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1. P N Page P N Page P N Page P N Page PHOO1 22 191 PHO0243 166 SP90133 176 SP90252D 134 PH00123 191 PH00252 167 SP90135 176 SP90252L 134 PHOO1 24 191 PHO0370 167 SP90144 189 SP90253D 134 PH00125 191 PH00371 167 SP90145 189 SP90253L 134 PH00126 191 PH00372 167 SP90146 189 SP90263 173 PH00127 191 PH00373 167 SP90147 189 SP90269 133 PH00128 172 PH00374 167 SP90160 205 SP90272 133 PH00129 172 PH00375 167 SP90161 205 SP90273 173 PH00130 172 PH00376 167 SP90164 134 SP90279 139 PH00131 172 PH00377 167 SP90166 134 SP90281 139 PH00132 172 PH00378 167 SP90167 134 SP90282 139 PH00133 172 PH00379 167 SP90168 201 SP90291 183 PH00134 172 PH00380 167 SP90169 201 SP90292 183 PH00146 167 PHO0381 167 SP90170 201 SP90293 183 PH00147 167 PH00382 167 SP90172 176 SP90294 183 PH00148 167 PH00386 165 SP90173 176 SP90295 183 PH00173 208 PH00388 165 SP90183 173 SP90320 133 PHOO1 74 208 PHO0389 165 SP90184 173 SP90321 133 PH00175 208 PH00390 165 SP90185 156 173 SP90322 182 PHOO1 76 208 PHO0391 165 SP90186 139 173 SP90323 198 PH00181 208 PH00393 165 SP90187 156 SPE10008 198 PH00183 205 PH00394 165 SP90188 156 SPFO1150 181 PH00184 205 PH00395 165 SP90189 156 SPFO1177 181 PH00185 205 PH00396 166 SP90190 156 SPG01649 178 PH00186 205 PH00397 166 SP90191 156 SPG01698 180 PH00187 205 PH00400 166 SP90192 156 173 SPGO2067 180 PH00188 205 PH00402 166 SP90193 156 173 SPGO2106 180 PH001
2. Product P N Page BGE USB XC1 30 SP90251 133 BGP TO BGE UPGRADE SP90235 134 BGP FWB GRAS20 1550 DESK SP90243D 133 BGP FWB GRAS20 1550 LAPTP SP90243L 133 BGP FWB GRAS20 DESKTOP SP90242D 133 BGP FWB GRAS20 LAPTOP SP90242L 133 BGP USB L11059 SP90320 133 BGP USB SP503 SP90236 133 BGP USB SP503 1550 SP90237 133 BGP USB SP620 SP90238 133 BGP USB SP620 1550 SP90239 133 BGP USB XC1 30 SP90241 133 BGS TO BGE UPGRADE SP90234 134 BGS TO BGP UPGRADE SP90233 134 BGS FWB GRAS20 DESKTOP SP90202D 133 BGS FWB GRAS20 LAPTOP SP90202L 133 BGS FWB GRAS20 1550 DESKTOP SP90203D 133 BGS FWB GRAS20 1550 LAPTOP SP90203L 133 BGS USB SP503 SP90197 133 BGS USB SP503 1550 SP90198 133 BGS USB SP620 SP90199 133 BGS USB SP620 1550 SP90200 133 BM USB SP503 SP90279 139 BM USB SP503 1550 SP90280 139 BM USB SP620 SP90281 139 BM USB SP620 1550 SP90282 139 Bracket for PD10 C PD10 pJ C PD10 IR pJ C 7208275 66 Bracket for PE9 C PE10 C PE1OBF C PE25 C PE25BF C 7208269 66 Bracket for PE50 C PESOBF C 72062 0 76 BT I SP90135 176 BT ll SP90133 176 BT I YAG SP90173 176 BI II YAG SP90172 176 Cable x PH00049 167 Carrying Case for Vega Nova lIl Nova and StarLite 1J02079 90 92 96 98 99 Case PH00209 210 CC PH00202 210 CFP PH00208 210 CM EXT10 PH00123 191 CM EXT25 PH00122 191 CM EXT40 PHOO121 191 CM EXT50 PHOO120 191 CM EXT100 PHOO119 191 C Mnt PHOO05 1 167 C NFP Assy SP90291 183 COL F
3. The Pyrocam Ill is extremely useful in the UV from 355nm to 157nm for 10 Excimer lasers and for tripled or quadrupled Nd YAG lasers The detector 0 1 1 10 100 is stable under UV illumination without the deterioration experienced by Wavelength in mm CCD cameras The pyroelectric detector operates in the visible spectrum Fig 6 Spectral response of Pyrocam Ill detector array and can see the alignment HeNe used with CO lasers However spurious AA response from the underlying silicon multiplexer creates undesirable performance and the camera is not recommended for quantitative visible measurements 3 2 4 ERRIMEN Er YAG laser at 2 9um Output of infrared fiber optic THz laser beam at 1 6THz 184um Free Electron laser at 100um Y OPHIR Y ie Photonics For latest updates please visit our website www ophiropt com photonics a 01 08 2013 A Newport Corporation Brand A Newport Corporation Brand wport Corpor Windows PC Interface The Pyrocam III Windows application incorporates setup software to control all functions roe an 111 Correa an oori alot x of the camera such as pulsed versus chopped operation gain and background reference Se ee ee subtraction eliminating all controls from the camera housing PChopoed Petbed Demierecsrti Pie RasDepiari Fam Doorsa mia jai i Moda E E MH iTA e e ie Whee aca m ela W
4. 65mm aperture a IPL version for IPL medical light sources ed N lt N Model L50 300 A L50 300 A LP1 L50 300 A PF 65 L50 300 A IPL a Use General purpose Long pulse lasers Large beam short Intense pulsed light agi pulsed lasers sources Absorber Type Broadband LE PF type LP1 coated window Spectral Range um 0 19 20 0 25 2 2 0 15 20 0 5 1 1 Aperture mm p 65mm p 65mm p 65mm p 65mm Power Mode Power Range 400mW 300W 400mW 300W 400mW 300W 400mW 300W Maximum Intermittent Power 300W for 2min 150W for 4 5min 50W continuous Power Scales 300W 30W 300W 30W 300W 30W 300W 30W Power Noise Level 20mW 20mW 20mW 20mW Maximum Average Power Density kW cm2 9at 300W 17 at 50W 23 at 300W 75 at 50W 3 20 Response Time with Meter 0 95 typ s 3 3 3 3 Power Accuracy 3 3 a 3 6 for most gel or air coupled IPL sources Linearity with Power 1 1 1 1 Energy Mode Energy Range 200m4J 300J 200mJ 300 200mJ 300J 120mJ 300J Energy Scales 300 60J 6J 300 60 6J 300J 605 6J 300 60J 6J Minimum Energy mJ 200 200 200 120 Maximum Energy Density J cm Single 10 50Hz lt 100ns 0 3 0 05 3 0 l5 0 05 Tus 0 5 0 3 3 9 eS 0 3 0 5ms 5 20 7 7 20 2MS 10 40 15 15 40 10ms 30 100 40 40 100 Cooling convection ballistic convection ballistic convection ballistic convection ballistic Weight kg 0 9 0 9 0 9 1 0 Version V1 Part number 7Z02658 7Z026415
5. A Newport Corporation Brand Newport Corporation Brand Water cooled a Up to 300W O g50mm aperture N Ss oD A O N Model L250W L300W LP 7 Use General purpose High power densities and m long pulses Absorber Type Broadband E Spectral Range um 0 19 20 0 4 1 5 10 6 Aperture mm p 50mm p 50mm Power Mode Power Range 1W 250W 4W 300W Power Scales 250W 30W 300W 30W Power Noise Level 50mW 200mW Maximum Average Power Density kW cm2 10at250W 14 at 100W 11 at 300W 14 at 150W Response Time with Meter 0 95 typ s 2 5 2 5 Power Accuracy 3 30 Linearity with Power 2 2 Energy Mode Energy Range 120mJ 200J 200mJ 300J Energy Scales 20037 3017 3 300 30 3 Minimum Energy mJ 120 200 Maximum Energy Density J cm lt 100ns Us 0 05 Tus 0 5 Os 0 5ms 5 20 2Ms 10 50 10ms 30 150 Cooling water water Minimum Water Flow Rate at Full Power 1 liter min 1 liter min Weight kg 0 6 0 6 Version Part number 7Z02688 7Z02689 Notes a Calibrated for 1 064um and 10 6um Notes b Water temperature range 18 30 C Water temperature rate of change lt 1 C min L250W L300W LP CABLE WATER CONNECTOR i 50 90 J p 1 4 20 BSW 6 deep l To a K 1 8 27 NPT THREAD FOR WATER CONNECTION WATER CONNECTOR FOR 91 4 PLASTIC HOSE 38 OU OPHIR 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics 1 1 2 6 High Power Water Cooled Thermal Sensors and Power
6. Description BeamMic software software license 2 format 640x480 pixel camera with 4 5mm CCD recess Comes with USB cable and 3 ND filters BM USB SP503 1550 BeamMic software software license 2 format 640x480 pixel camera with 4 5mm CCD recess Phosphor coated o 1550 nm Comes with USB cable and 3 ND filters BM USB SP620 BM USB SP620 1550 BeamMic software software license 1 1 8 format 1600x1200 pixel camera with 4 5mm CCD recess Comes with USB and cable and 3 ND filters BeamMic software software license 1 1 8 format 1600x1200 pixel camera with 4 5mm CCD recess Phosphor coated to 1550 nm Comes with USB and cable 3 ND filters Software Upgrades BeamMic to BGS Upgrade Upgrade BeamMic to BeamGage Standard Edition Requires a camera key to activate SP cameras may require a firmware upgrade to enable ROI features BeamMic to BGP Upgrade Upgrade BeamMic to BeamGage Professional Edition Requires a camera key to activate SP cameras may require a firmware upgrade to enable RO features BeamMic to BGE Upgrade Optical Synch for Pulsed Lasers Upgrade BeamMic to BeamGage Enterprise Edition Requires a camera key to activate SP cameras may require a firmware upgrade to enable ROI features Optical Trigger for SP Cameras Recommended Optional LBS 300 BB Optical trigger assembly which can be mounted on camera or separately to sense laser pulses and synchronize SP
7. 3 0 EERME Results Window User Notes Status Bar Primary Dock Window note tabs ee Q OPHIR Photon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport A Newport Corporation Brand Brand A Newport Corporation Brand Integrated Power Meter ri The silicon and germanium NanoScan2 systems now come with an integrated 200mW power meter The relative power meter provides 1 5 correspondence to a user supplied measurement when configured in the same geometry as calibrated It comes with a quartz attenuator of power within the window that provides a uniform response across a broad aperture integrated power wavelength range measurement calibrated with customer power sensor The power meter screen in the software shows both the total power and the individual power in each of the beams being measured aE Available Detectors lB The NanoScan 2 is available with either silicon or germanium to cover the light spectrum from UV to infrared The scan heads are available in several sizes apertures and slit dimensions See the table for available configurations NanoScan Scanhead Model Si 3 5 1 8um Si 9 5um Si 9 25um Wavelength 190nm 950nm 190nm 950nm 190nm 950nm Detector Silicon Silicon Silicon Entrance Aperture 3 5MM 9mm 9mm Slit Size 1 8um 5um 25um 1 e Beam Diameter Range 7um 2 3mm 20um 6mm 100um
8. Laser tuning screen and power and energy log 2 USB and RS232 interfaces with StarLab and StarCom PC applications v LabVIEW driver COM Object Interface and Activex control see pages 105 109 VU m Soft keys and menu driven functions with on line help gt Many software features such as density min max scaling etc T The Vega is the most versatile and sophisticated handheld laser power energy meter on the market Just plug in one of the many Ophir lt sensors and you have a whole measurement laboratory at your fingertips The bright color display gives unparalleled legibility and ease of interpreting information The Vega has many on board features such as laser tuning data logging graphing normalize power or energy an density units attenuation scaling max and min limits The Vega can also display the power or energy with a high resolution simulated analog needle display i The Vega can be operated either by battery or from an AC source with en 2 825mW z the charger plugged in at all times Its bright display and backlit keys O allow easy use in dark room conditions or with laser glasses on SO oi mern Sa m TTT PPNI PAT RAR yyy The built in USB and RS232 interfaces and StarLab and Starcom PC p i y ET on PERCEKA G CEEKIE i software allow on line processing of data or processing previously are 7 E stored data results are displayed graphically on a PC To support S en il PC interfacing LabVIEW drivers COM Object Interfac
9. 2 3 3 EONS AVGE Ophlstrd llb Library supplied for use with the Dual Channel LaserStar Communication can be set to RS232 or GPIB and is based on NI VISA Ophinstr llb This library can be configured to work with the Nova ll Vega USB Interface or Single Channel LaserStar devices It can also work with the Juno with a Thermopile or Photodiode sensors It can be set to RS232 USB or GPIB It is based on NI VISA for all 3 communication protocols Therefore to work with it in USB first run the SwapINF utility that we provide to configure your PC to replace the USB drivers supplied by Ophir with drivers supplied by National Instruments Library supplied for use with all of our USB speaking devices Juno Nova ll Pulsar USBI Vega eer a 5 LabVIEW COM Demo llb Makes use of our COM object Included with our StarLab application 2 OPHIR a For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand rt Corporatio 2 4 OEM Power Meter Solutions 2 4 1 Examples of Custom OEM Power Energy Meter Solutions In addition to the standard products described above Ophir has accumulated over 25 years experience in developing products which are tailored to precise physical configurations provided by the OEM customer These products include special display software options OEM power energy meter board sets and much more A number of these special OEM products are shown below Mov
10. 97 14 ADJUSTABLE 3A FS 625 19 REMOVABLE PART i M20x1 x 4 deep 923 97 14 ADJUSTABLE 1 75 3A P FS 12 ABSORBER SURFACE WINDOW 6 8 8 5 97 143 ADJUSTABLE 1 75 For latest updates please visit our website www ophiropt com photonics 1 1 2 1 High Sensitivity Thermal Sensors 2mW to 12W Features m Very low noise and drift to measure very low powers and energies 12A 12A P Broadband and P absorbers for CW and A short pulses Up to 12W G Spectrally flat a9 N m N Model 12A 12A P r Use General purpose Short pulses Absorber Type Broadband P type Spectral Range um 0 19 20 013 0 Aperture mm 16mm 16mm Power Mode Power Range 2mW 12W 2mW 12W Power Scales 12W to 20mW 12W to 20mW Power Noise Level 50uW 50uW Thermal Drift 30min 40 150uW 40 150uW Maximum Average Power Density kW cm 25 0 05 Response Time with Meter 0 95 typ s 25 35 Power Accuracy 2 3 Linearity with Power 1 5 1 5 Energy Mode Energy Range 1mJ 30J 1mJ 30J Energy Scales 30J to 30mJ 30J to 30mJ Minimum Energy mJ 1 1 Maximum Energy Density J cm Pulse rate Single 10 30Hz lt 100ns 0 3 10 1 0 5MS 5 10 2ms 10 10 1 10ms 30 10 Cooling convection convection Fiber Adapters Available see page 44 ST FC SMA SC SU FC OMA SG Weight kg 0 35 0
11. A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand Newport Corporation Brai BeamGage See your beam as never before 3 2 1 G 3 2 1 1 BeamGage Standard Version Extensive set of ISO quantitative measurements Patented Ultracal algorithm for highest accuracy measurements in the industry Customizable user interface for ease of use Auto setup and Auto exposure capabilities for fast set up and optimized accuracy Statistical analysis on all calculated results displayed in real time New BeamMaker beam simulator for algorithm self validation The performance of today s laser systems can strongly affect the success of demanding modern laser applications The beam s size shape uniformity or approximation to the expected power distribution as well as its divergence and mode content can make or break an application Accurate knowledge of these parameters is essential to the success of any laser based endeavor As laser applications push the boundaries of laser performance it is becoming more critical to understand the operating criteria For over thirty years Ophir Spiricon has developed instruments to accurately measure critical laser parameters Our LBA and BeamStar software have led the way Now with the introduction of BeamGage Ophir Spiricon offers the first new from the ground up beam profile analysis instrument the industry has experienced in over 10 years BeamGage include
12. ACTIVE AREA 7 1 x 5 4 DUAL IEEE 1394b PORTS 17 5 ACTIVE AREA TRIGGER SERIAL PORT Firewire Cameras for use with Laptop or Desktop PC Item Specification Model GRAS 20 Application 1 1 8 format high resolution CW YAG adjustable ROI Spectral Response Maximum beam size Pixel spacing Number of effective pixels Minimum system dynamic range Linearity with Power Accuracy of beam width Frame rates Shutter duration Gain control Trigger Photodiode trigger Saturation intensity Lowest measurable signa Damage threshold Dimensions and CCD recess Image quality at 1064nm Operation mode Software supported PC interface Minimum host system requirements 190 1100nm 7 1MM W x 5 4mm H 44um x 44um 1600 x 1200 61dB 1 2 15Hz full res gt 60Hz depending on ROI From 1 frame rate to 1 10 000s Manual or continuous automatic control Odb to 25db Manual control Supports both trigger in and strobe out Optional photodiode trigger available ESP GRAS 0 3uW cm 0 4nW cm2 50W cm 1J cm with all filters installed for lt 100ns pulse width 35mm x 44mm x 65mm Fixed C mount Pulsed with video trigger good Pulsed sync excellent CW good Interline transfer progressive scan CCD BeamGage IEEE 1394b Firewire IEEE 1394b requires 1394b port or PCI Express or CardBus Slot 01 08 2013 Notes 1 Camera set to full resolution at maximum frame rate and equivalent
13. Hard drive space suitable to hold the amount of video data you expect to store 50 100 GB recommended Provision for PCI Express FireWire USB2 or Gigabit Ethernet input depending on camera Interface hardware provided with a cameras except USB2 3 2 1 4 ERMENI 132 Y OPHIR Y Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Ga Corporation Brand A Newport Corporation Brand Newport Corporation Brand Ordering Information Item Description P N BeamGage Standard USB2 Beam Profiler Systems camera and software BGS USB SP503 BeamGage Standard software software license 1 2 format 640x480 pixel camera with 4 5mm CCD recess SP90197 Comes with USB cable and 3 ND filters BGS USB SP503 1550 BeamGage Standard software software license 2 format 640x480 pixel camera with 4 5mm CCD recess SP90198 Phosphor coated to 1550 nm Comes with USB cable and 3 ND filters BGS USB SP620 BeamGage Standard software software license 1 1 8 format 1600x1200 pixel camera with 4 5mm CCD SP90199 recess Comes with USB and cable and 3 ND filters BGS USB SP620 1550 BeamGage Standard software software license 1 1 8 format 1600x1200 pixel camera with 4 5mm CCD SP90200 recess Phosphor coated to 1550 nm Comes with USB and cable 3 ND filters BeamGage Standard FireWire Beam Profiler Systems camera and softw
14. She alee any tans tj Pukar Pind 2e iad ache Pir L Sers i Mhobeckodh PINON inir GAY Guus Therrecgile BP N iS OF far STS as E E pE l Yi iE 4 871mW fE 43 00mw amas Lactang fra LSE deve Dre Ciba hirii Cele Cees H Setup Screen Choose line graph Choose sensor settings Choose display and graph settings or bargraph I Choose sensor functions L lt a E 9 131 w T rer or needle display r 1 I r 1 T z r 1 T i i T 2 i Dehi Cees ma AOON 0 j One of above screens maximized OU OPHIR Phatianics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Bran Multiple sensors displayed together Click on one of the channels The settings and scale are from channel chosen ee ll i Bfe yeu Log Selec ere Meveced chore Core girde te OLF EELK Ti i r i Eri ila a ee ee G Here multi line graph display has been chosen Settings and functions may be opened to adjust then minimized as needed GPG eH Boe ee Boe ed See ee cee RAFE Pe ee eee 2 3 1 Genera leitelas LP Hint LA g fan Bo ALa Fas Lc Ha i LL hrii Ha Mle F TAi m itd Bae wha l r Pias J 2a haan ae J 140 5u sears odin heise E Pare A pa o GBR EE BE
15. 1 8 4 ADJUSTABLE T THREAD SIZE 135 180 ADJUSTABLE 1 4 BSW 2x QUICK CONNECT FITTING 135 180 TE EE R RESER FOR 93 8 PLASTIC HOSE FOR 63 8 PLASTIC HOSE ji 75 100 Bo o v 75 100 01 08 2013 2 OPHIR Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 1 1 2 6 High Power Water Cooled Thermal Sensors and Power Pucks 20W to 10kW Features Comet power pucks measure heat rise from 10s exposure to laser Accurate built in temperature compensation algorithm Up to 10kW Up to 100mm apertures Model Use Absorber Type Spectral Range um Aperture mm Power Mode Power Range Repeatability Maximum Average Power Density kW cm2 Power Accuracy Linearity with Power Number of readings before probe must be cooled for 25 C starting temp Maximum Energy Density J cm lt 100ns 10us Ims 10ms Time to Reading Temperature Compensation Maximum Permitted Probe Temperature Display Operation Mode Comet 1K Comet 10K Comet 10K HD UA w Y YU UY O Comet 1K Comet 10K Comet 10K HD N For powers to 1kW For power
16. 1460 1470 1480 1490 1500 1510 1520 1530 1540 1550 1560 1570 1580 1590 1600 1610 Wavelength nm Phosphor Coated Cameras with Spiricon s BeamGage software Spiricon s engineers have carefully measured the non linearity of the signal generated by the Phosphor Coated series cameras The software in the BeamGage incorporates an algorithm to correct for the non linearity This illustration shows the linearity obtained showing in the top line that the low level signals drop linearly rather than at the square of the input seen in the lower line The two photos show the uncorrected and corrected camera beam shape in 3D See the BeamGage section for additional information on the beam analyzer Beam profile of a fiber beam with Beam profile of a fiber beam without 34 non linearity correction non linearity correction ACTIVE AREA 6 5 x 4 8 a 37 1 32 UN C Mount BNC CONNECT SP 1550M RS 170 monitor display when used without a frame grabber Y OPHIR D Spiricon Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand Newport Corporation Brand 3 2 3 4 MASE 45 01 08 2013 Specifications Phosphor Coated For NIR Response Model SP503U 1550 SP620U 1550 GRAS20 1550 SP 1550M Application NIR wavelengths 12 format NIR wavelengths 1 1 8 for NIR wavelengths 1 1 8 NIR wavelengt
17. 1 3 4 Wyelaiseras 01 a 2 o HIR __ Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand 1 3 5 StarLink Direct to PC Energy Sensors The StarLink Energy Sensor Series The StarLink series is a select group of Ophir energy sensors that are provided with the Ophir Juno USB PC interface attached The StarLink sensor is connected via a USB cable to the PC USB port and can then operate directly with the PC with no need for an Ophir power meter The StarLink package comes bundled with the celebrated Ophir StarLab software the easiest to use and most sophisticated power energy meter PC software available Alternatively StarLink sensors can be operated from the user s software via the COM Object interface provided or can work with LabVIEW via the drivers provided 1 3 5 REALL For more details about the computer interface options and StarLab software see section 2 3 1 on page 105 Below is a list of the StarLink energy sensors currently available together with the reference page for the specifications on the relevant sensor StarLink Sensor StarLink P N Corresponding Ophir P N Data sheet page stand alone sensor PE10 C StarLink LES VS Pie ORC TZQ29352 66 PE25 C StarLink 78 156 PE25 C 7202937 67 PE25BF C StarLink 78 154
18. 15 Output Beam either to power meter or to Beam Dump User selectable ND filters for attenuating input to the camera Focal Spot Assembly showing various beam paths Y OPHIR Y Spiricon Photonics For latest updates please visit our website www ophiropt com photonics Soy eee ES 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport A Newport Corporation Brand Brand Examples of Usage 65um diameter focal spot Focal spot shape changing with laser power level Specifications Model YAG Focal Spot Analyzer Wavelength 1064nm Wedge Material BK7 Wedge Coating AR lt 1 Clear aperture 17 5mm Wedge ND value each ND 2 ND Filters Bulk ND ND Values nominal 0 3 7 1 0 2 0 3 0 4 0 Red holders Filter Slides 3 Filter Damage 50 W cm 1J cm 10ns pulse Negative Lens FSA 50Y To add FSA capability 50mm YAG FSA 100Y 100mm YAG FSA 125Y 125mm YAG FSA 150Y 150mm YAG FSA 200Y e 200mm YAG NN Accessories a Variable Wedge ND Filter kit WVF 300 a0 Beam Dumps BD 040 A 40 Watts Max Power Air Cooled z BD 500 W 500 Watts Max Power Water Cooled lt Note 1 ND bulk absorbing filters damage threshold is 50W cm but should be used at lt 5W cm to avoid thermal lensing effects Ordering Information W aa Item Description P N YAG Focal Spot Analyzer m YAG Focal Spot Analyzer assembly requires 1 each LBS 300 NIR and 1 each Negative Lens lt p LBS 30
19. Beam position and wander All the other features of standard power energy meters OU OPHIR Photonics N ae U m Many software features such and density min max scaling etc The Nova Il is the most versatile and sophisticated handheld laser power energy meter on the market Just plug in one of the many Ophir sensors and you have a whole measurement laboratory at your fingertips The Nova Il has many on board features such as laser tuning data logging graphing normalize power or energy density units attenuation scaling max and min limits The Nova II can also display the O power or energy with a high resolution simulated analog needle display O The Nova Il can be operated either by battery or from an AC source with N the charger plugged in at all times Its backlight allows illumination ofthe PE 205 0uW r S x The built in USB and RS232 interfaces and StarLab and StarCom PC i software allow on line processing of data or processing previously stored data results are displayed graphically on a PC To support PC interfacing 7 LabVIEW drivers Com Object Interface and ActiveX controls are provided 1 Hi i StarLab Software Standard Power Screen Sensor type Access further and S N Range iy S functions aser gt 800 Average NONE Selected range Average period Selected laser l length Can average ove
20. In addition to finding the right sensor for your application the Sensor Finder Program offers the following features Report printing How close the recommended sensors are to the specified damage threshold Order of Selection 1 0 BSfelaisrelas The sensors are selected in terms of cost effectiveness and ease of use i e photodiode sensors and thermopiles are selected first and then pyroelectric and RP sensors If you want to measure only power pyro and RP sensors will not be selected even if they could operate within all other given laser parameters If you select a repetition rate consistent with single shot energy lt 0 2Hz RP sensors will not be selected even if they could operate within all other given laser parameters Aperture Since it is not practical to allow the beam to fill the entire aperture the sensors are selected so that the sensor aperture is always at least 2mm or 10 larger than the beam If the beam is rectangular its corners can touch the aperture Using the Sensor Finder Program The Sensor Finder Program is available for use online at www ophiropt com sensor finder It can also be downloaded for use on your own PC at www ophiropt com sensor finder download Sensor Finder Input Screen Step 1 Step 2 Mantuirement Type Enter Laser Parameters L ti ni mT r CUN i Pulsed Aret PpS mm j Energy Ranga Mn is Maw F 1 in ti m xi Beam ese Carcular Power Range Min lo Maa C a Beer Deus C R
21. OPHIR Photonics A Newport Corporation Brand Optional Automation Interface The Pro model scanheads implement an Automation Server that can be used by an Automation Client written in Visual Basic for Applications VBA C C or by an application with support for Activex Automation such as Microsoft Excel Microsoft Word or National Instruments LabVIEW NanoScan Acquisition and Analysis Software Feature NanoScan Standard NanoScan Professional all features in Standard plus Controls Source ScanHead Select Gain Filter Sampling Resolution AutoFind Rotation Frequency Record Mode Capture Averaging Rotation Magnification CW or Pulse Modes Divergence Gaussian Fit Reference Position Recompute 7 Regions of Interest ROI Single or Multiple Automatic or Manual Colors Profiles Vertical Scale 17 10 100 Logarithmic Scale Z amp PAN Automatic or Manual Computation ISO 13694 ISO 11146 Dait 13 5 50 2 User Selectable Clip Levels Dao Width ratios Centroid Position Peak Position Centroid Separation Peak Separation Irradiance Gaussian Fit Ellipticity ig Divergence Total Power Pulse Frequency power Continuous Rolling Finite Pointing Centroid or Peak Accumulate Mode Beam Indicator Graph Center Colors ji 2D 3D 2D or 3D Mode Linear or Logarithmic Scale Resolution Fill Contours Solid Surface or
22. Off axis delivery optics m Figures 5 amp 6 show an industrial Nd YAG laser with misaligned turning mirror before and after adjustment Alignment of devices to lenses m Figures 7 amp 8 show beam profiles during alignment of a collimating lens to a laser diode The first profile shows poor alignment of the lens to the diode which can easily be improved when seeing the profile in real time Laser amplifier tuning m Figures 9 amp 10 show a Cr LiSAF femtosecond laser oscillator beam with a near Gaussian output and what happens to the oscillator beam with poor input alignment All these examples illustrate the need for beam monitoring 1 4 CERME Measurement of the beam profile is needed to know if problems exist and the profile must be seen to make corrections Most laser processes can be improved Scientific experiments can be more accurate Commercial instruments can be better aligned Military devices can have greater effectiveness Industrial processing produces less scrap Medical applications are more precise Just knowing the beam profile can make the difference between success and failure of a process 116 D OPHIR Spiricon Photon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics 2 S OPHIR Photonics OPHIR Photonics A Newport Corporation Brand wport Corporation Brand A Newport Corporation Brand A Newport Corporation Brand 3 2 In
23. excellent CW good Inline transfer progressive scan BeamGage Enterprise Gigbit ethernet PC desktop with PCI Express slot or laptop with PCI Express 34 slot Windows 7 32 64 or Vista 32 74 A N gt C lt Q wal Notes 1 Camera set to full resolution at maximum frame rate and equivalent exposure times running CW at 632 8nm wavelength Camera set to minimum useful gain for saturation test and maximum useful gain for lowest signal test 2 The maximum rate depends on the ROI Region of Interest size the bits readout and the number of cameras on the same bus The SCOR 20 operates at 7 5Hz 12 bits and 15Hz 8 bits It operates up to at least 60Hz with a smaller ROI The frame rate also depends on PC resources 3 May be usable for wavelengths below 350nm but sensitivity is low and detector deterioration may occur Therefore UV image converter is recommended Although our silicon cameras have shown response out to 1320nm it can cause significant blooming which could lead to significant errors of beam width measurement We would suggest our XC130 InGaAs camera for these wavelengths to give you the best measurements 4 This is the damage threshold of the filter glass of the filters Assuming all filters mounted with ND1 red housing filter in the front Distortion of the beam may occur OU OPHIR Photonics For latest updates please visit our website www ophiropt com photonics A Newpor
24. 01 08 2013 GENERAL SPECIFICATIONS FOR PYROCAM III FEATURES a Firewire to PCI adapter a Windows image viewer 2D and 3D beam display Readout externally calibratable for energy or power Frame averaging and summing for low level signal analysis Data logging Manual gain setting Plus calculations previously provided X amp Y width Centroid location Peak location Total power or energy in digital counts Windows setup menu control console no buttons or knobs more user friendly High speed up to 1kHz standard Automatic lock in to pulse trigger rate Programmable exposure time to reduce signal loss from thermal spread 50us to 12 8ms in 50us increments Slider for fine adjustment gain settings 1X to 10X CW 6X Pulse User enabled bad pixel correction Separate bad pixel correction for pulsed and CW User enabled gain correction separate for pulsed and CW Internet field upgradeable firmware Interface to 3rd party software via ActiveX Export images in omp or ASCII file format Ordering Information Item Description P N Pyrocam III Beam Profiler Systems PY III P A Pyroelectric array detector pulsed only Grade A two FireWire ports and basic viewer software BeamGage SP90090 Standard included To complete this order you must add an Interchangeable Window part number to accompany this system see below PY III P B Pyroelectric array detector pulsed only Grade B two Fi
25. 200sM FW A 1000 1300nm lens 11402 001 OU OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand Y Spiricon OPHIR Photonics A Newport A Newport Corporation Brand poration Brand For latest updates please visit our website www ophiropt com photonics 3 6 1 1 oSelaawavarel asic 189 01 08 2013 3 6 1 2 EERME 190 3 6 1 2 Model 1780 Instantly measure M The ModeScan Model 1780 is a laser beam profiling instrument that measures the M Beam Propagation Ratio and all associated ISO 11146 parameters instantaneously in real time at video rates to over 20Hz The measurement technique patented by Photon Inc uses 10 reflective surfaces to form simultaneous images of the propagating beam at 10 locations on a Model 2512 CCD array camera With all ten measurement positions acquired at once the instrument is suitable for measurement of both CW and pulsed lasers down to single shot rates Beam diameters are obtained with NIST traceable accuracy to better than 2 using the BeamPro This translates to M measurements with accuracy to 5 The FireWire system operates under Photon s BeamPro in Microsoft Windows The compactness of the system and the IEEE 1394a FireWire interface offers enhanced ease of use and portability The ability to operate in any orientation allows for easy placement on any optical bench and saves valuable bench space The CCD is sensitive from 250nm to 1100nm wavelengths T
26. 50A PF DIF 18 30A N 18 s4 DATS He ADJUSTABLE ADJUSTABL ais 140 Ji 100 OU OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand 1 1 2 3 Bxelawserss 32 01 08 2013 1 1 2 3 Low Medium Power Thermal Sensors Apertures to 35mm 30mW to 150W Features Convection air cooled CW to 30W or 50W intermittent to 150W m 17 5mm and 35mm apertures 30 150 A BB 18 30 150 A LP1 18 L50 150 A BB 35 L50 150 A LP1 35 L50 150 A PF 35 Model 30 150 A BB 18 30 150 A LP1 18 L50 150 A BB 35 L50 150 A LP1 35 L50 150 A PF 35 Use General purpose High power density General purpose High power density Short pulse lasers and long pulse lasers and long pulse lasers Absorber Type Broadband LPI Broadband LP PF Spectral Range um 0 19 20 0 25 2 2 0 19 20 0 25 2 2 0 15 20 Aperture mm p 17 5MM p 17 5MM p 35MM 35MM 35MM Power Mode Power Range 30mW 150W 30mW 150W 100mW 150W 100mW 150W 100mW 150W Maximum Intermittent Power W 150W for 1 5min 100W for 2 2min 150W for 1 5min 100W for 2 5min 50W continuous 30W continuous Power Scales 150W 30W 3W 150W 30W 3W 150W 50W 5W 150W 50W 5W 150W 50W 5W Power Noise Level 2mW 2mW AmW AmW AmW Maximum Average Power Density kW cm2 12at150W 20at30W 38at150W 97at30W 12 at SOW 17at50W 38 at 150W 75 at 50W 3 Response Time with Meter 0 95 typ s 1 2 1 2 2
27. 5Vdc LVTTL TTL positive or negative user programmable Minimum pulse width 10us Trigger Out External Trigger cable provided Voltage Requirement Power Consumption 3 3Vdc LVTTL Programmable Powered over Firewire Cable lt 3 5watts Dimensions 44mm 1 74 wide 29mm 1 14 tall and 66mm 2 6 deep Mass 104g 3 702 Environmental Storage Temperature 30 C to 65 C Storage Humidity 95 maximum non condensing Operating Temperature 10 C to 40 C Operating Humidity Power Requirements 95 maximum non condensing Line Voltage 95V AC to 250V AC Line Frequency 47Hz to 63Hz Maximum Power 4 5 Watts For the Optical Train only The PC computer supplies the power for the system components such as the CCD camera An external power supply is provided for Laptop computer use Physical Weight M 200s 6 8 kg without camera Measurements Mex My Kx Ky BPPx BPPy Statistical results Width at waist Wx Wy are available on Divergence angle qx ay all measurements Waist location Zx Zy Rayleigh X Y Astigmatism Wavelength Range Asymmetry ratio Different lenses are needed for different wavelength regions The M 200s model include 3 standard lenses with nominal 300mm focal lengths See below M 200s FW 266 587nm included 400 750nm included 650 1125nm included 1000 1300nm optional Attenuation Range Nominally from ND 0 to ND 4 8 Actual values vary with waveleng
28. It has a response time of 50ms and power capacity of 100W Ordering Information The products shown above are examples of OEM solutions developed for specific customer applications Please consult with your Ophir representative who will be happy to help you with any requirements you may have 01 08 2013 _ 2 OPHIR a For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand ration Brai 1 2 BeamTrack Power Position Size Sensors Ophir now has the new BeamTrack line of thermal sensors that can measure beam position and beam size while measuring power This innovative device will provide an additional wealth of information on your laser beam centering beam position beam wander beam position and wander beam size as well as power and single shot energy The BeamTrack sensor is illustrated schematically here and works as follows the signal coming from the sensor is divided into 4 quadrants so by measuring and comparing the output from the 4 sections we can determine the position of the center of the beam to a high degree of accuracy In addition to the 4 quadrants there is now a special patented beam size detector After processing outputs from these various detectors the user is presented with the beam position as well as beam size Note that the beam size is calibrated only for Gaussian beams but for other beams it will give relative size information and will indicate if the beam is changing
29. LPK CO 16 0 5 3X 3 0 16mm 10 6um 0 5 beam splitter assorted attenuators Pyrocam Ill LPK CO 16 5 0 3X 3 0 16mm 10 6um 5 beam splitter assorted attenuators Pyrocam Ill ga on Ordering Information Item Description P N fee LPK CO gt 6 4 0 5 BGS PC PIll software Pyrocam Ill with chopper PY III C B 10 6 LBS 100 IR 0 5 beam splitter attenuator base plate SP90075 miscellaneous hardware Suitable for beams 1 0 to 6 4mm M LPK CO gt 6 4 5 0 BGS PC PIll software Pyrocam Ill with chopper PY III C B 10 6 LBS 100 IR 5 0 beam splitter attenuator base plate SP90076 miscellaneous hardware Suitable for beams 1 0 to 6 4mm F LPK CO 16 0 5 BGS PC PIll software Pyrocam Ill with chopper PY III C B 10 6 LBS 100 IR 0 5 beam splitter attenuator 3X telescope SP90077 base plate miscellaneous hardware Suitable for beams 3 0 to 16mm LPK CO gt 16 5 0 BGS PC PIll software Pyrocam III with chopper PY III C B 10 6 LBS 100 IR 5 0 beam splitter attenuator 3X telescope SP90078 base plate miscellaneous hardware Suitable for beams 3 0 to 16mm Maximum beam size assumes zero diffraction from the wings of the beam Beams of up to 1 5X the maximum size can be applied with minimal diffraction Beams of up to 2X the above size can be applied but noticeable diffraction will occur 202 Y OPHIR Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photoni
30. NS Pyro 20 25 NS Pyro 20 25 SP620 NIR 1000 0 1100nm L11059 NS Ge 12 25 NS Pyro 20 25 Z WN 1500 1600nm 3P 620 1550 XEVA XEVA 5P 620 1550 5P 620 1550 NS XEVA Z WN WN VA VA D 40 oD aya J q Abbreviations FIR Far Infrared NIR Near Infrared Ge Germanium Si Silicon HP High Power SP Indicates camera profiler MIR Mid Infrared NS NanoScan UV Vis Ultraviolet Visible Q OPHIR Spiricon Photon For latest updates please visit our website www ophiropt com photonics See OLS 2018 ewport Corporation Bran jewport Corporation Bran ewport Corporation bran 3 1 4 Benefits of Beam Profiling You can get more out of your laser m Figure 1 shows an industrial Nd YAG laser near Gaussian beam with 100 Watts output power and 1 5kW cm 2 power density Figure 2 is the same Nd YAG beam at greater power 170 Watts but it split into 2 peaks producing only 1 3kW cm2 power density The power density of the beam decreased 13 instead of increasing by the 70 expected Without measuring the beam profile and beam width you would not know what happened to your power density and why the performance did not improve Laser cavities become misaligned m Figures 3 amp 4 are beam profiles of CO lasers used for ceramic wafer scribing in the same shop The second laser with the highly structured beam produced mostly scrap parts until the laser cavity was aligned
31. Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 01 08 2013 1 1 2 Thermal Power Sensors 30uW to 3W Features 1 1 2 1 High Sensitivity Thermal Sensors 3A 3A P 3A P THz 3A FS 3A P FS 12 N Very low noise and drift to measure O very low powers and energies N Broadband and P absorbers for CW and short pulses T m Upto 3W a Spectrally flat Version for Terahertz N e Model 3A 3A P 3A P THz 3A FS 3A P FS 12 a Use General purpose Short pulses Calibrated for With removable For divergent Terahertz window beams window radiation blocks infrared Absorber Type Broadband P type P type Broadband FS P type F S window window Spectral Range um 0 19 20 0 15 8 0 3 10THz 0 19 20 0 22 2 1 Aperture mm p 9 5MM p 12mm p 12mm p 9 5MM p 12mm Maximum Beam Divergence NA NA NA NA 40 degrees Power Mode Power Range 60uW 3W 60uUW 3W 50uW 3W 30uW 3W 60uUW 3W Power Scales 3W to 300UW 3W to 300UW 3W to 300uW 3W to 300uW 3W to 300uW Power Noise Level 2uW 4uW 4uW 2uW 6uW Thermal Drift 30min 5 20uW 5 30uW 5 30uW 2 10uW 20 40uW Maximum Average Power Density kW cm2 1 0 05 0 05 1 0 05 Response Time with Meter 0 95 typ s 1 8 2 5 2 5 1 8 2 5 Power Accuracy 3 3 15 3 3 Linearity with Power 1 5 1 5 1 5 1 5 1 5 Energy Mode Energy Range 20u 2 20uJ 2J 20uJ 2J 15uJ 2J 20uJ 2J Energy Scales 2J to 2
32. StarLab 2 10 and higher that allows the system integrator to take control of the Juno Nova ll Pulsar USBI and Vega devices integrating them into his in house measurement and analysis package For communication via USB device drivers and additional support software must be installed on your PC These components are installed as part of the StarLab application s installation process System Integrators will need the following components m OphirLMMeasurement COM Object doc lists and describes the methods and events available for configuring controlling and uploading measurements from Ophir devices m OphirLMMeasurement dll COM object component developed and supplied by Ophir for communication with the Juno Nova ll Pulsar USBI and Vega devices The COM object is registered when the application is installed OphirL_MMeasurement COM Object doc describes how to register it on another PC where the Ophir application has not been installed m Standard USB cable for use with the Pulsar and USBI devices included m Standard mini B USB cable for use with the Juno device included Nova ll Vega USB cable P N 7E01 205 for use with the Nova ll and Vega devices included with the Nova II Vega Ophir provides example projects of COM Object clients in VC VB NET and LabVIEW These are found in the Automation Examples subdirectory of our StarLab PC Application Note The OphirFastX for Pulsar devices as well as the OphirUsbX for Nova
33. format slim profile 1 1 8 format high 1 1 8 format high 1 1 8 format high 36mm x 24mm 35mm wide dynamic range resolution wide resolution CW YAG resolution networkable format for large beams CW amp pulsed dynamic range adjustable ROI long cable distances CW YAG Adjustable ROI lasers adjustable ROI pulsed lasers CW YAG adjustable ROI adjustable ROI Number of Elements 640 x 480 1600 x 1200 1600 x 1200 1600 x 1200 4008 x 2672 Interface Style USB USB Firewire 1394b Gigbit Ethernet USB Windows 05 support Windows 7 32 64 Vista 32 64 or XP 32 Pro Windows 7 32 64 or Windows 7 32 64 Vista Vista 32 64 32 64 or XP 32 Pro 1440 1605nm A Ca 2a 2 Model SP503U 1550 SP620U 1550 GRAS20 1550 al Spectral Response nm 1440 1605nm 1440 1605nm 1440 1605nm Application NIR wavelengths 2 format NIR wavelengths 1 1 8 NIR wavelengths 1 1 8 low resolution format low resolution format adjustable ROI adjustable ROI and binning se Number of Elements 640 x 480 1600 x 1200 1600 x 1200 Q Interface Style USB USB Firewire 1394b aa Windows 05 support Windows 7 32 64 Vista 32 64 or XP 32 Pro q T 13 355nm amp 1 06 3000um Ci 900 1700nm H MM Model XEVA 100Hz Model Pyrocam III Spectral Response 900 1700nm Spectral Response nm 13 355NM amp 1 06 3000uMm Application High resolution InGaAS performance Application UV amp Far IR NIR wavelengths Number of Elements O 56 N
34. histograms and more Monitor up to 7 Quasars simultaneously on one PC Quasar Bluetooth Wireless Sensor to PC Interface Quasar module connects to any Ophir sensor thermal Any PC or laptop connects to Quasar module via Bluetooth pyroelectric or photodiode Specification adapter and operates as a power energy meter data logger 2 2 3 GReiele NAteltelas Sensor Compatibility Number of Sensors on One PC Operating Range Power LED Indicator Bluetooth Standard Data Transfer Rate for Pyro Sensors Dimensions Connections All Ophir standard sensors thermal photodiode and pyroelectric Up to 7 Quasars can operate simultaneously and be displayed at the same time on one PC 10 30 meters depending on surroundings when used with built in laptop Bluetooth or Ophir recommended adapter Powered by rechargeable NiMH battery Battery life typical 40 hours 20 hours for pyro sensors Automatically goes into sleep mode when not connected to PC Low batt indication Charges from 12VDC either polarity The charger can be ordered from your local distributor LED indicator indicates whether connected in standby or off Bluetooth class 1 Connection to PC is transparent to user Will work with built in laptop Bluetooth and most add on USB to Bluetooth adapters Ophir recommended USB to Bluetooth adapter Ophir P N 7E10039 see table below 500Hz 96mm W x 95mm D x 36mm H not including antenna 15 pin D type sensor connector standard Ophir
35. information for further details 3 4 4 ERRIMEN Y OPHIR Y Spiricon Photonics For latest updates please visit our website www ophiropt com photonics Se eee ES 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport A Newport Corporation Brand Brand PERAEEE FE Shown is an image of the tip of a single mode fiber UV converter of 9um diameter The beam width as measured on assembly for 4X the profiles shows 4X the actual size so we see a Beam Expander resolution of 2um Approximate Spectral range Distance from lens Distance from Distance of closest Total length of expansion ratio barrel to focus focus to 1tbeam approach to focus assembly splitter with 1 beam splitter 4X 400 1800nm 8mm 18mm 32MM 50mm 6X 600 1064nm 16mm 10mm past 1 surface 4 5mm 107mm 12X 600 1064nm 6mm 6mm 20mm 101mm 22X 600 1064nm 24mm 8mm 22mm 102mm Ordering Information Item Description P N 4X reimaging beam expander Screw optical assembly that images the plane 8 mm in front of the expander onto the CCD SPZ17022 while enlarging it 4X Fits 4 5mm recess and CS mount cameras Y Fiber adapter bracket for 4X beam expander Screw on bracket to use with Ophir fiber adapters so fiber is held in correct position to image SPG01649 N fiber tip onto camera Will give exact focus with FC type fiber D UV converter assembly for 4X beam expander Screw on assembly which has UV plate that conver
36. of given values Note c With the user threshold setting set to minimum For other settings the spec is for gt 7 of full scale or greater than twice the user threshold whichever is greater The user threshold is available with Nova Il Vega StarLite or Juno For other meters the threshold is set to minimum and the linearity spec is gt 10 of full scale The PE C series will only operate with Nova or Orion meters with an additional adapter Ophir P N 7Z08272 see page 77 The adapter can introduce up to 1 additional measurement error The user threshold feature allows adjustment of the internal threshold up to 25 of full scale if desired to avoid false triggering in noisy environments The user threshold setting represents the approximate minimum energy for pulse widths below 50 of the pulse width setting For longer pulse widths the actual minimum may be higher For highest accuracy it is recommended to zero the sensor against the meter the first time it is used with a particular meter For further information see the FAQs on our Website Note d A shock absorbing mounting post is available for situations in which sensor is mounted on a surface subject to shock or vibration This can prevent false triggering and allow working at lower minimum energies Note however that in this case the maximum average power will be reduced to 10W without heat sink and 20W with heat sink see accessory pages 76 77 for heat sink and mounting post Note e
37. range of travel A Mitutoyo micrometer with a handy re zeroing feature and accompanying slide provides precise determination of the scan head location and or travel distance with a resolution of tens of microns For automated and automatic M measurements the NanoModeScan option is required Pulsed Laser Beam Profiling In addition to profiling CW laser beams NanoScan can also profile pulsed laser beams with repetition rate in the 1kHz range and above To enable the measurement of these pulsed lasers the NanoScan profiler incorporates a peak connect algorithm and software controlled variable scan speed on all scanheads The accuracy of the measurement generally depends on the laser beam spot size and the pulse to pulse repeatability of the laser The NanoScan is ideal for measuring Q switched lasers and lasers operating with pulse width modulation power PWM control In the past few years lasers with pico and femtosecond pulse durations have begun to be used in many applications Although these lasers add some additional complication to the measurement techniques the NanoScan can also measure this class of laser Optional Power Meter 3 3 1 ERMENE The silicon and germanium NanoScan systems offer the 200mW power meter as an option The power meter can be calibrated against the user s ISO or NIST traceable power meter The 200mMW power meter has a quartz attenuator window that provides a uniform response across a broad wavelength ra
38. with filter installed 01 08 2013 1 1 1 3 Special photodiode sensors and integrating spheres 1 1 1 3 1 Special Photodiode Sensors Features BC20 PD300 BB for broadband light sources radiometry i PD300 BB 50mW option up to 50mW C Pp Ta PD300 CIE for eye adjusted Lux measurements ee O BC20 for measuring scanned beams such as bar code light sources N T PD300 BB PD300 BB 50mW PD300 CIE lO M i Model PD300 BB PD300 BB 50mW PD300 CIE BC20 Use Radiometry broad Same as PD300 BB with removable Eye adjusted Scanned beams e g bar code spectrum attenuator for use to 50mW measurement in Lux Detector Type Silicon with special filter Silicon with special filter Silicon with special filter Silicon with peak and hold circuit Aperture 10x10mm 10x10mm Active area 2 4x2 8mm 10x10mm Spectral Range nm 430 1000 see graph 430 1000 see graph 400 700 see graph 633 650 675 others available Filter Mode Filter out Filter in Power Range 4mW to 50pW 4mW to 50pW 50mW to 1nW 200kLux to 20 mLux 20mW to 100uW Power Scales 4mW to 8nW anddBm 4mWto8nWand S50mWto80nW 200kLux to 200 mLux 20mW to 2mW dBm and dBm Resolution nW 0 001 0 001 0 01 1 mLux 0 001 Accuracy Maximum deviation from Maximum deviation from flat see graph 3 for gt 10 of full scale flat spectrum see graph spectrum see graph Deviation from calibration 3 at 10 10 12 30 000 inch s scan rate on sensor Damage Threshold W cm2 10 10 100
39. 00 1000e 00 2580e 05 Watts bhar aa a E a bjr Geode i ues Peak Fhence 80 9003 03 9398 03 4 169e 00 Watis on a ee m DhE Min Fluence 0 437e 0i 4795p 0 14 he 0 Watson Figa Garii Erez Paplea TopHat Eff Pwr 160 7279e 01 73316 01 Lez5e 4 Watts i incr Tap Spatial GT Mam Ciad thescription Vahue Miran Sti Dey Unite Centred GO 519999 320000 OCOD um PORET aaa i Centoid Y SO 739003 739001 000 um meen a H PeaklocX ISO 298000 318927 20075 ome 3 Peak Loc Y SO 27000 241714 0430 eter rl 4 i Mla 141395 141409 O00 um hi E a E Daat 141400 141409 0000 um _ conor into her 141403 141409 ofo6 um pee dye Weri T ch eth Depkx 719000 134m0 ORS urn shining i 1 F qT DHpkY 1M000 133154 g pi um A F d D 4 3 T p Ti w o R Cursors With Power Processing Status 3D Beam Display Buffered Video Energy Readouts Indicators Scrolling Controls LD Beam Results With 1D Profiling Options Statistics ISO Compliant Results Pass Fail with Password Protection for Production Testing BeamGage allows the user to configure the displayed calculations set up the screen layout and password protect the configuration from any changes This permits secure product testing as well as data collection for Statistical Process Control SPC all while assuring the validity of the data Spatial Carte eter 1a Pilea Sed Dr Miss Mlin lhara Centroki K 150 36013335e 03 75115
40. 1 06micron wavelength Software includes Activex automation feature PH00429 PH00430 PH00431 NS2 Ge 3 5 1 8 PRO NS2 Ge 9 5 PRO NS2 Ge 9 25 PRO NanoScan2 Si Detector 9mm aperture 5micron slits High resolution head featuring Si detector 63 5mm diameter head with rotation mount 9mm entrance aperture and matched pair of 5 micron wide slits Use from 190nm to wavelengths lt 1micron Not for 1 06micron wavelength Software includes Activex automation feature NanoScan2 Si Detector 9mm aperture 25micron slits High resolution head featuring Si detector 63 5mm diameter head with rotation mount 9mm entrance aperture and matched pair of 25 micron wide slits Use from 190nm to wavelengths lt 1micron Not for 1 06micron wavelength PHO0432 PH00433 PH00434 3 0 FERMAS Q OPHIR Photon Photonics For latest updates please visit our website www ophiropt com photonics SR O O08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand 3 3 1 UxSeiaawalarciais 158 01 08 2013 3 3 1 NanoScan Scanning Slit Beam Profiler For High Accuracy Dimensional Measurement NanoScan is a PC based instrument for the measurement and analysis of optical beam spatial profiles in accordance with ISO standards Beam profiles are measured using the International Standard ISO 11146 Scanheads that are fitted with an optional power feature can measure power in accordance with ISO
41. 1 2 4 Wylalaweras 34 01 08 2013 1 1 2 4 Medium Power Large Aperture Thermal Sensors Apertures 50mm 100mW to 150W Features Thin profile CW to 35W or 50W intermittent to 150W a 50mm aperture For continuous long pulse and excimer lasers L40 150 A L40 150 A LP1 L40 150 A EX L50 150 A Model L40 150 A L40 150 A LP1 L40 150 A EX L50 150 A Use General purpose Long pulse lasers Excimer lasers General purpose Absorber Type Broadband LP1 EX Broadband Spectral Range um 0 19 20 0 25 2 2 2 94 0 15 0 7 10 6 0 19 20 Aperture mm p 50mm p 50MM p 50MM 50mm Power Mode Power Range 100mW 150W 100mW 150W 100mW 150W 100mW 150W Maximum Intermittent Power 150W for 3min 80W for 5 5min 35W continuous 150W for 4min 100W for 6min 50W continuous Power Scales 150W 20W 150W 20W 150W 20W 150W 20W Power Noise Level 5mW 10mW 5mW 5mW Maximum Average Power Density kW cm 12 at 150W 20 at 35W 38 at 150W 90 at 35W 2 12 at 150W 17 at 50W Response Time with Meter 0 95 typ s 2 5 25 2 5 25 Power Accuracy 3 a0 3 3 Linearity with Power 1 1 1 1 Energy Mode Energy Range 100mJ 200J 100m4J 300J 100mJ 200J 100mJ 300J Energy Scales 200J 30J 3J S007 307 3 ZOO SO 3 300 30 3J Minimum Energy mJ 100 100 100 100 Maximum Energy Density J cm lt 100ns 0 3 0 05 OS 03 Tus 05 0 3 0 6 0 5 0 5ms 5 20 6 5 2MS 10 50 12 10 10ms 30 250 25 30 Cooling convection ballistic convection ballis
42. 10 50 Max Pulse Energy uJ 1 1 10 1 NA Noise Level pW 2 2 30 ae gay 5uW Response Time with Meters 0 2 0 2 0 2 0 2 Two modes of operation Hold holds highest reading for 5s then updates No Hold updates reading 3 times per second Beam Position Dependence 2 for broadband light 2 for broadband 3 for NA source overfills E Sources light sources broadband light detector Sources Background Subtraction NA NA NA NA Background is automatically subtracted from both scanned and static beams Fiber Adapters Available NA SC STFC SMA NA NA see page 43 Version Part Number 7Z02405 7Z02440 7Z02406 7Z02422A Notes a Swivel stand for BC20 sensor P N b The PD300 CIE and BC20 sensors are not fully supported by Ophir PC Interfaces Juno USBI Pulsar and Quasar or by StarLite Meter 1209004 For graphs see page 24 PD300 BB CIE PD300 BB PD300 BB 50mW with filter installed BC20 PD300 BB 50mW with filter off 118 119 5 10 st I lt l y Bottom View Bottom View a j Front View 17 8 Front View 9 5 Front View 01 08 2013 7 2 OPHIR Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 1 1 1 3 2 Special Sensors Integrating Spheres 1uW to 3W Features Integrating sphere for diver
43. 13694 The system comprises a scanhead for sensing the laser beam a USB 2 0 controller and NanoScan software An optional automation feature includes an Activex automation server NanoScan uses moving slits one of the ISO Standard scanning aperture techniques Measurement is possible for beam sizes from microns to centimeters at beam powers from microwatts to over kilowatts often without attenuation Detector options silicon germanium and pyroelectric technologies allow measurement at wavelengths from the ultraviolet to the far infrared It can simultaneously measure multiple beams and offers an optional power meter for scanheads with silicon and germanium detectors Profiles are acquired with 12 bit digitization and analyzed for real time updates up to the maximum scanhead scan rate of 20Hz With NanoScan beam profile measurement is extremely easy simply position the scanhead in the beam path and within seconds the system does the rest Benefits m All NanoScan systems are calibrated to a NIST traceable source to ensure the ultimate in accuracy m The software finds a beam in less than 0 3 seconds and displays real time updates up to 20Hz m The Z axis datum plane of the NanoScan is known to 25um making the locating of beam waist position simple and accurate Along with the ability to measure pulsed beam diameters the NanoScan accurately measures and reports the pulse frequency of the laser ensuring that the pulsed beam measu
44. 15 3um 10 6um 120uJ 10J 250Hz 15 PE50 DIF C Pyroelectric with diffuser high repetition rate O35mm 0 19 3um 20uJ 10J 10 000Hz 75 we StarLink Complete calibration curve ee PESOBF DIF C Pyroelectric with diffuser for highest damage O35mm 0 19 2 2um 200uJ 10J 250Hz 79 StarLink threshold Complete calibration curve 2 94um Y Ss aD e VY Energy Sensor Accessories O Accessories for pyroelectric sensors Ka Fiberoptic adapters Accessory Description Page Pyroelectric F O Adapters Adapters for mounting fibers to pyroelectric sensors ST FC SMA SC 76 Accessories Accessory Description Page Removable Heat Sink Heat sink that is fastened to rear of PE C sensors Allows average power 50 70 higher than without heat sink 76 Scope Adapter Plugs in between the PE sensor and power meter Provides BNC output to scope to see every pulse up to the maximum 76 frequency of the sensor Beam Splitter Assembly Beam Splitter Assembly to measure pulsed laser sources too energetic for direct measurement Use with the Beam 76 Splitter can be calibrated by setting the laser to a lower energy that will not damage the sensor and swiveling between position A and B and then taking the ratio of A and B Shock Absorbing Mounting post same size as standard but with rubber shock absorber to insulate PE sensor from vibrations 77 Mounting Post Nova PE C Adapter The adapter plugs between the Nova D15 socket and the smart plug of the PE C sensor to allow the Nova to operate n wit
45. 150 A SV 17 Very high damage threshold 30W O17mm 0 19 12uUm 100mMW 150W 50m4J 300J a3 continuous 150W intermittent 30 150 A HE 17 High energy and average power YAGs and harmonics 17mm 0 19 0 625um 50mW 150W 60mJ 2005 33 30W continuous 150W intermittent 1 064um 2 1m 2 94um 30 150 A HE DIF 17 For highly concentrated Q switched pulses to 30W O17mm 0 19 3um except for 50mW 150W 60mJ 2005 33 intermittent to 150W 625 900nm Medium power thermal sensors apertures 50 to 65mm 100mW 300W Sensor Features Aperture Spectral Range Power Range Energy Range Page L40 150 A CW to 35W intermittent to 150W large aperture O50mm 0 19 20um 100mW 150W W 100mJ 200J 34 L40 150 A LP1 As above high damage threshold for long pulses O50mm 0 25 2 2um 2 94um 100mMW 150W 100mJ 300J 34 L40 150 A EX As above for excimer lasers O50mm 0 15 0 7um 10 6um 100mW 150W 100mJ 200J 34 L50 150 A CW to 50W intermittent to 150W O50mm 0 19 20um 100mMW 150W 100mJ 300J 34 L50 300 A CW to 50W intermittent to 300W very large aperture 65mm 0 19 20um 400mW 300W 200mJ 300J 35 L50 300 A LP1 As above high damage threshold for CW and long pulses 65mm 0 25 2 2UM 400mW 300W 200mJ 300J 35 L50 300 A PF 65 CW to 50W intermittent to 300W large beam short pulses 65mm 0 15 20um 400mW 300W 200mJ 300J 35 L50 300 A IPL For gel coupled IPL sources 65MM 0 5 1 1um 400mW 300W 120mJ 300J 35 Medium high power fan cooled thermal sensors 50mW 500W Sensor Features Aperture Spectral Range Power Range
46. 181 2nd Wedge Beam Splitter SPZ17026 177 3A 7 Z02621 28 3A FS LZ02628 28 3A FS StarLink 76 002 28 42 3A IS 7ZO2404 2 3A IS IRG 7 Z02403 27 3A P 7 Z02622 28 3A P FS 12 7Z02687 28 3A P QUAD 7Z07935 56 3A P StarLink 78 001 28 42 3A P THz 7202742 28 3A QUAD 7Z07934 56 3A QUAD StarLink 787203 42 56 3A StarLink 78 000 28 42 3CustomFxt PHOO214 210 3D PHOO206 210 3D LED PHOO207 210 3LED Mount PHOO211 210 3W Mount PH00216 210 4mm spacer SPG01698 180 4X reducing UV image converter SPZ17024 181 4X reimaging beam expander SPZ1 022 178 4X reimaging beam reducer SPZ17017 179 5mm spacer SPGO2106 180 6X expanding microscope objective SPZ08257 178 8mm spacer SPG02067 180 10A 7202637 30 10A P 7ZO02649 31 10A PPS 7207904 56 10A PPS StarLink 78 7202 42 56 10A StarLink 78 004 30 42 10K W 7Z02645 40 10kW SH V2 7ZO02645 204 10X SP90295 183 12A 7202638 29 12A P 7Z02624 29 12X expanding microscope objective SPZ08259 178 15 50 A PF DIF 18 7Z02740 31 20C A Consult Ophir representative 49 20C SH 7 Z02602 49 20C UAU Consult Ophir representative 49 20mm diameter UV imaging plate SPFO1177 181 20X SP90294 183 22X expanding microscope objective SPZ08260 178 25mm focal length CCTV lens kit SP90085 180 30 150 A BB 18 7202699 32 0 150 A BB 18 StarLink 78 007 32 42 30 150 A HE 17 ZQ02 22 33 30 150 A HE DIF 17 7202729 33 0 150 A LP 1 18 72027215S 32 30 150 A SV 17 7ZO02724 33 30A BB 18 7202692 30 30A BB 18 StarLink 787006 30 42 30A N 18 7202695 31
47. 2 2 Power Accuracy 3 ae 3 3 9 4 Linearity with Power 1 1 1 1 1 Energy Mode Energy Range 20mJ 100J 20mJ 300J 40m 300J 40mJ 3005 DOU 300 Energy Scales NOON SON 3 300 7 30 73 300J 30J 3J S00 7 30U7 3 300J 30J 3J Minimum Energy mJ 20 20 40 40 50 Maximum Energy Density J cm Singel 18 50Hz lt 100ns 0 3 0 05 0 3 0 05 30 BS 0 5ms 5 20 5 20 7 yi 2ms 10 50 10 50 15 15 10ms 30 250 30 250 40 40 Cooling convection ballistic convection ballistic convection ballistic convection ballistic convection ballistic Fiber Adapters Available see page 44 ST FC SMA SC ST FC SMA SC ST FC SMA SC ST FC SMA SC ST FC SMA SC Weight kg 0 3 0 3 0 35 0 35 35 Version Part number Standard Sensor 7Z02699 7Z02721S 7Z02730 7Z02726S 7Z02737 StarLink Sensor Direct USB link to PC p 42 787007 Note a LP1 sensors have relatively large spectral variation in absorption and have a calibrated spectral curve at all wave lengths in their spectral range to the above specified accuracy Nova and Orion meters do not support this feature and when used with those meters accuracy will be 3 for 532nm 808nm 1064nm and 2100nm and 6 for other wavelengths in the spectral range 400 1100nm 30 150 A BB 18 30 150 A LP1 18 L50 150 A BB 35 L50 150 A LP1 35 L50 150 A PF 35 49 g 66 i 29 24 13 15 ey os i 9 ADJUSTABLE
48. 200 2m 2m 2m m 2m Oe om amd Lowest Measurable Energy uJ 8 10 60 80 100 60 100 120 120 200 Max Pulse Width ms 0 002 0 03 0 5 1 5 1 2 5 10 20 Maximum Pulse Rate pps 1OkHz 5kHz 900Hz 450Hz 100Hz 250Hz 100Hz 50Hz 40Hz 20Hz Noise on Lowest Range yJ 0 5 1 6 10 20 10 20 20 20 40 Additional Error with Frequency t2 to 15 2 to 15 to 15 to 1 1 1 1 2 5kHz 4 750Hz 400Hz 80Hz to 10kHz Linearity with Energy for gt 7 of full scale e 596 2 Damage Threshold J cm lt 100ns 0 1 0 8 lus 0 2 1 300us 2 5 2Ms 6 10 Maximum Average Power W 15 25 with optional heat sink 15 25 with optional heat sink Maximum Average Power Density W cm 20 20 Uniformity over surface 2 over central 50 of aperture 2 over central 50 of aperture Fiber Adapters Available see page 76 ST FC SMA SC ST FC SMA SC Weight kg 025 0 25 Version Part Number Standard Sensor 7Z02937 7Z02935 StarLink Sensor Direct USB link to PC p 75 787156 787154 Note a Calibration curve is verified and adjusted at specified wavelengths Specified wavelengths 248 266nm 355nm 1064nm Specified wavelengths 193nm 248 266nm 355nm 532nm and 2940nm 1064nm and 2940nm At other wavelengths there may be an additional error up to the value given Max additional error at other wavelengths 2 Max additional error at other wavelengths 2 Note b For wavelengths below 600nm derate damage threshold to 60 of given values Below 300nm derate to 40
49. 2D and 3D power density The disadvantage is that the ModeCheck must be positioned further from the distribution output head in order to properly recreate the collimated beam profile The re collimating lens must be supplied by the user and must be the same lens that is used on the lasers cutting head See application note SP90329 A PC is required to run the ModeCheck imaging software The camera is powered over the USB cable that connects the computer to ModeCheck Y OPHIR Y Spiricon Photonics For latest updates please visit our website www ophiropt com photonics Soy eee ES 01 08 2013 A Newport Corporation Brand A Newport Corporation Brand Specifications Model ModeCheck Laser Input Power 50 5000 Watts Input Clear Aperture 50mm 2 Beam Width 5mm 30mm Pick off Percent 0 5 1 2 4 10 sampling wands user replaceable Damage Threshold 27 36 W cm2 See graph Camera 1 3 format CMOS 640x480 6um pixel 8bit CS mount USB2 Lens 25mm C mount Cooling Built in Fan water required for the optional beam dump or optional power meter sensor UV Light Source LED array Software ModeCheck v5 0 Power Requirements Input 100 240 Vac 50 60Hz 1 5A Output 12Vdc 5 0A w power jack UL listed and CE compliant universal power supply included Camera is powered over the USB port Dimensions 9 5 X13 x 6 7 242mm x 330mm x 171mm The optional rugged case is recommended Not including handle
50. 30W heat sinked 30W 5W 30W 3W 1mW AmW 20 at 30W 28 at 10W 20 at 30W 28 at 10W 0 8 1 5 3 3 1 1 6mJ 30J 20m4J 60J 30 3J 300mJ 60J 20J 2J 200mJ 6 20 0 3 0 3 2 5 2 10 2 30 convection convection conduction ST FC SMA SC NA 0 3 0 1 7Z02692 7Z02273 787006 30A BB 18 ITS ae L L30A 10MM 75 01 08 2013 a Photonics A Newport Corporation Brand Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics 1 1 2 2 Low Power Thermal Sensors 40mW to 50W Features m Convection air cooled m P PF and N type absorbers 10A P 30A P 17 15 50 A PF DIF 18 50A PF DIF 18 30A N 18 for short pulses 16mm to 17 5mm apertures C Q 15 50 A PF DIF 18 al Model 10A P 30A P 17 50A PF DIF 18 30A N 18 NI Use Short pulse to 10W Short pulse to 30W High energy density High power density pulsed beams pulsed YAG N Absorber Type P type Pipe Fy be cimusey N type m Spectral Range um 0 15 8 0 15 8 0 24 2 2 0 532 1 064 p Aperture mm 16mm p 17mm o 17 5MM 17 5MM Power Mode Power Range 40mW 10W 60mW 30W 140mW 50W
51. 35 Version V1 Part number 7Z02638 7Z02624 Notes a Depending on room airflow and temperature variations Notes b For the 30mJ energy scale measurements it is recommended to use the screw on barrel supplied with the sensor to protect from direct air flow Note c For P type and shorter wavelengths derate Wavelength Derate to value maximum energy density as follows 1064nm Not derated 532nm Not derated 355nm 40 of stated value 266nm 10 of stated value 193nm 10 of stated value 12A 12A P 16 j 25 REMOVABLE PART M20x1 x 4 deep 19 45 J ADJUSTABLE 107 150 75 L T00 J Q OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand 1 1 2 2 Low Power Thermal Sensors 20mW to 150W Features m Convection air cooled Broadband absorber Spectral Range um Aperture mm Power Mode Power Range Maximum Power a 16mm to 26mm apertures Fast response time Y VU UY N moda i se N Absorber Type Power Scales Power Noise Level Maximum Average Power Density kW cm Response Time with Meter 0 95 typ s Power Accuracy Linearity with Power Energy Mode Energy Range Energy Scales Minimum Energy mJ Maximum Energy Density J cm lt 100ns 0 5ms 2Ms 10ms Cooli
52. 50mm lens A o1 A Oo EEr oe D oO aN O oO o1 wo Ol N z Detector to Lens spacing S NO Sz Detector to lens spacing amp O N O SSS SSS SS SS Sees a ee ie Ee ea ey a E e SR et E a Es N E S ee SS E m Ee Ee EE Ee aS SSS Sars Bla SS ae aE SE i Re a eh ei Se a ae Rs ee ee A Ee a a re ESS ESS eS Ee Ee ee E SR E SS Bes Be Bais SS ee ee ee es ee SS See Se cis Ss ES a a ea ht 3 4 6 ERRIMEN Poo Zec 2cc00O0OOnC Conca MATT OR PUEH OOHOOH T o CECE oone gongon Hoop ong HOPE Oooo COSCO PAn I i a a __ IW D La A LAG LA H AA DY EEN N i __ a E E aa pa A 15 4 15 TEES ss Sts Sa 0 100 200 300 400 500 600 700 800 900 1000 1100 Aa io TE aai aes Lens to Object spacing Beam reduction X Ordering Information item Description p Ee p _ o P N 25mm focal length CCTV lens kit 25mm focal length lens assembly with locking iris and focus adjustment Includes 1 ea 8mm spacer and SP90085 2 ea 5mm spacers 50mm focal length CCTV lens kit Same as above except 50mm focal length lens SP90038 4mm spacer Screw on spacer to add 4mm spacing to optical system SPGO1698 5mm spacer Screw on spacer to add 5mm spacing to optical system SPG02106 8mm spacer Screw on spacer to add 8mm spacing to optical system SPG02067 1
53. 5kHz 900Hz A50Hz 100Hz 250Hz 100HzZ 50Hz 40Hz 20Hz Noise on Lowest Range uJ 1 2 20 20 40 15 30 40 40 60 Additional Error with Frequency 2 to 2 1 to 2 to 1 to 1 1 1 1 2 2kHz 750Hz 400Hz 80Hz 4 5 to 5kHz Linearity with Energy for gt 7 of full scale 1 5 2 Damage Threshold J cm lt 100ns 3 Tus 2 5 300us 20 25 2ms 40 50 Maximum Average Power W 20 30 with optional heat sink 20 30 with optional heat sink Maximum Average Power Density W cm2 100 120 Uniformity over surface 2 5 over central 20mm 2 5 over central 10mm Weight kg 0 25 0 25 Version Part Number Standard Sensor 7Z02939 7Z02941 StarLink Sensor Direct USB link to PC p 75 787157 Notes a Calibration curve is verified and adjusted at specified Specified wavelengths Specified wavelengths wavelengths 193nm 248 266nm 1064nm 2100nm and 2940nm 193nm 248 266nm 355nm 532nm 1064nm and 2100nm At other wavelengths there may be an additional error up to Additional error at 193nm 6 Max additional error at other Additional error at 193nm 6 the value given wavelengths not specified above 2 Max additional error at other wavelengths not specified above 193nm reading may need 1min irradiation to stabilize 3 193nm reading may need 1min irradiation to stabilize Notes b For wavelengths gt 2um derate to 10 of above values For wavelengths below 600nm derate to 60 of given values For beam size lt 5mm For 10mm beam derate to 5
54. 60mW 30W Maximum Intermittent Power W NA NA for 15 50 A PF DIF 18 only NA 50W for 5min 15W continuous Power Scales 10W 2W 200mW and dBm 30W 3W 50W 5W 30W 3W Power Noise Level 2mW 3mW 7mW 3mW Maximum Average Power Density kW cm 0 05 0 05 0 5 5 Response Time with Meter 0 95 typ s 3 5 2 5 2 2 Power Accuracy 3 3 5 3 Linearity with Power 1 5 i gt 15 1 Energy Mode Energy Range 10mJ 10J 40mJ 30J 60mJ 200J 30mJ 200J Energy Scales O 200i 2O 2007ra WO 307 3 Minimum Energy mJ 10 40 60 30 Maximum Energy Density J cm Pulse rate Single 10 30Hz Single 10 30Hz 10 30Hz O 0H lt 1us 10 1 10 1 4 1 0 5ms 10 1 10 1 is 20 5ms 10 1 10 1 50 gt 100 Cooling convection convection convection convection Fiber Adapters Available see page 44 ST FC SMA SC ST FC SMA SC NA ST FC SMA SC Weight kg 0 2 0 3 0 35 0 3 Version V3 Part number 7Z02649 7Z02693 7Z02740 7Z02738 7Z02695 Note a For shorter wavelengths derate maximum Wavelength Derate to value Wavelength Derate to value energy density as follows 1064nm Not derated 1064nm Not derated 532nm Not derated 532nm 80 of stated value 355nm 40 of stated value 355nm 60 of stated value 266nmM 10 of stated value 266nM 40 of stated value 193nm 10 of stated value 193nm NA 10A P 30A P 17 15 50 A PF DIF 18 37 o 16 260 64 M20x1 x4 deep DAT e n l 6 EA 2 ADJUSTABLE ma 90 130 ADJUSTABLE 2x M3 x 3 deep aS 95 140 95 140 a k 75 100 100 a e 100
55. 6mm Spatial Sampling Resolution 5 3nm 18 3um 5 3nm 18 3um 5 3nm 18 3um Profile Digitization 16 bit 16 bit 16 bit Scan Frequency 1 25 2 5 5 10 20Hz 1 25 2 5 5 10 20Hz 1 25 2 5 5 10 20Hz Power Aperture User calibrated User calibrated User calibrated Power Aperture OD Metallized Quartz 200mW Metallized Quartz 200mW Metallized Quartz 200mW Laser Type CW or Pulsed CW or Pulsed CW or Pulsed Operating Range See Operating Space Chart in Appen See Operating Space Chart in Appen See Operating Space Chart in Appen dix C of User s Manual dix C of User s Manual dix C of User s Manual Damage Threshold see Operating Space Chart in Appen See Operating Space Chart in Appen See Operating Space Chart in Appen dix C of User s Manual dix C of User s Manual dix C of User s Manual Rotation Mount Standard see drawing in Appendix B Standard see drawing in Appendix B Standard see drawing in Appendix B of User s Manual of User s Manual of User s Manual Scanhead Dimension See Mechanical Drawing in Appendix See Mechanical Drawing in Appendix See Mechanical Drawing in Appendix of User s Manual B of User s Manual B of User s Manual 1 Assumes Gaussian TEM00 Beam 2 Pulsed Operation Limited to Beam Diameter gt 100uUm and pulse repetition rate gt 5kHz NanoScan Scanhead Model Ge 3 5 1 8um Ge 9 5um Ge 9 25um Wavelength 700nm 1800nm 700nm 1800nm 700nm 1800nm Detector Germanium Germanium Germanium En
56. 875 1749 3499 GERM Diameter 9 389 778 1555 3110 M 10 350 700 1400 2799 O E 11 318 636 1272 2545 lt i eee a a deai Seis Tee AL Weel 12 292 583 1166 2333 fiir Niel eowupe maieiaifi 190 40Gren erealencl 13 269 538 1077 2153 jimi Badangd nicka aperture materia 14 250 500 1000 1999 15 233 467 933 1866 16 219 437 875 1749 17 206 412 823 1646 18 194 389 778 1555 19 184 368 737 1473 20 175 350 700 1400 21 167 333 666 1333 2 159 318 636 1272 23 152 304 608 1217 24 146 292 583 1166 25 140 280 560 1120 50 70 140 280 560 h A High Power NanoScan with cooling fan Q OPHIR Photon Photonics For latest updates please visit our website www ophiropt com photonics E OS 108 2013 A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand High Power NanoScan Configurations DetectorType Power Range Wavelength Aperture Slits Scan Head Size Pyroelectric IV oy 190nm gt 9mm SUM 100mm upper limit 100um dependent on wevelength Pyroelectric al Wace 190nm gt 20mm 10um 100mm Large Aperture upper limit 100um dependent on wevelength High Power NanoScan Ordering Information High Power NanoScan All High Power NanoScan Systems Include Fan cooled scanhead For use at wavelengths from 200nm to greater than 20um Maximum power capacity is dependent on wavelength and spot size Refer to operating space charts for more information Slits and scan drum are highly reflectiv
57. AX reducing UVimage Screw on imaging telescope that converts UV image to visible reduces the size 4X and images on CCD For beam SPZ17024 converter intensities from 1uJ cm to 15mJ cm2 Beam splitter for above 45 degree wedged beam splitter to reduce intensities on by 20X For beam intensities of up to 300mJ cm2 at 193mm SPZ17007 UV converter assembly Screw on assembly which has UV plate to convert 193 360nm radiation to visible The plate is at the object plane of SPZ17019 for 4X beam expander the 4X expander P N SPZ17022 and produces a 4X enlarged image on the CCD 20mm diameter UV 20mm diameter UV image conversion plate only For customers that have own imaging system Converts UV SPFO1177 imaging plate image to visible For beam intensities 50uJ cm to 10uJ cm 30mm diameter UV 30mm diameter UV image conversion plate only For customers that have own imaging system Converts UV SPFO1150 imaging plate image to visible For beam intensities 50uJ cm to 10uJ cm 50mm X 50mm UV 50X50mm diameter UV image conversion plate only For customers that have own imaging system Converts UV SP90082 imaging plate image to visible For beam intensities 1mJ cm to 20mJ cm Not suitable for 193nm 100mm X 100mm UV 100X100mm diameter UV image conversion plate only For customers that have own imaging system Converts UV SP90083 imaging plate image to visible For beam intensities 1mJ cm 2 to 20mJ cm2 Not suitable for 193nm
58. Applied Option Pixel scale settings Magnification settings Ultracal Frame buffer settings Enable Auto X auto exposure control Perform an Auto Setup 8 10 12 14 16 bits per pixel Select Format or ROI Measure S N ratio Capture methods are features related to the application while Synchronization methods relate more to the abilities of the specific camera NOTE Frame capture rates are determined by many factors and are not guaranteed for any specific operating configuration Q OPHIR Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand P Spiricon OPHIR Photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand Features BeamGage Standard BeamGage Professional BeamGage Enterprise all features in Standard plus all features in Pro plus Trigger modes a CW captures continuously see Capture Options below Trigger In from laser Trigger pulses supplied to the camera a Strobe Out to laser Strobe pulses output from the camera a Video Trigger Frame captured and displayed only when the camera sees a signal greater than a user set level Capture options l Capture options are redefined and are approached in a different manner than older products The items listed below will allow for all of the previous methods but with more flexability than ever befo
59. Brand 3 2 1 4 Software Comparison Chart Features BeamGage Standard BeamGage Professional BeamGage Enterprise all features in Standard plus all features in Pro plus Features Overview User selectable for either best accuracy or ease of use Supports our patented Ultracal algorithm plus Auto setup and Auto exposure capabilities Extensive set of ISO quantitative measurements Support for USB Firewire and Pyrocam Ill cameras Supports InGaAs cameras in Supports Gig E camera in Firewire cameras limited to 32bit OS only 32bit OS only both 32 and 64 bit OS Support for USB Firewire and Pyrocam Ill InGaAs GigE New Beam Maker beam simulator for algorithm self validation See below for more detailed description Simultaneous 2D and 3D displays Multi instance multi camera use Supports networked USB Firewire and Pyrocam Ill cameras Gig E in a future release Results synchronised to select models of Ophir power energy meters Supported products include Vega Nova Il Pulsar USBI and Juno in both 32 and 64bit OS Quasar is not supported Supports Satellite windows on multiple monitors Continuous zoom scaling in both 2D and 3D Window partitioning to allow analysis of multiple beams on a single camera Camera ROI support on USB and Firewire cameras Manual and Auto aperturing to reduce background effects Pass Fail on all results items w multiple alarm options Beam Pointing Stability
60. Configuration Files ASCII file Profiles and Summary Parameters Raw 3D Scan Data in binary format Screen Captures BMP JPG GIF TIFF PNG Log to Files and COM Ports Communications RS 232 Serial COM port required Activex Automation Electrical Mechanical AC Power Required 110V 60Hz standard 220V 50Hz optional Installation Category Class Il Main supply voltage fluctuations Not to exceed 10 of the nominal voltage Transient overvoltage according to Installation Category Il Pollution Degree 1 or 2 in accordance with IEC 664 Dimensions mm Scanning Unit 318 X 228 x 241 Scanner 203 x 165 x 165 Motion Controller 51 X 89 x 248 Environmental Conditions Indoor use Temperature 5 C 40 C Altitude Ut 2000 Maximum relative humidit 80 for temperature up to 31 C decreasing linearly to 50 relative humidity at 40 C OU OPHIR Photon For latest updates please visit our website www ophiropt com photonics OPH Phoronis A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand 3 9 FERMAVE 207 01 08 2013 3 9 EERME 208 01 08 2013 Ordering Information Goniometric Radiometer Far Field Profilers All Goniometric Radiometer LD 8900 Far Field Profiler Systems include the Scan Unit PCI Controller Interface Current MS Windows software including Activex Automation commands All LD 8900R systems include the above as well as a dynamic range gt 36dB with OdB
61. FEZ SPs VAOIO35 67 PE50 C StarLink 787 55 PE50 C 7202936 68 PES0BF C Starlink rola PESOBF C 7202934 68 PE50 DIF C StarLink 787157 PE50 DIF C 7202939 69 PES50BF DIF C StarLink 787 158 RESOBRHEDIHEE 7202940 70 Q OPHIR 2 Photonie For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand 1 3 6 Energy Sensors Accessories 1 3 6 1 Accessories for Pyroelectric Sensors Fiberoptic Adapter for Oscilloscope Adapter for Heat Sink for Pyroelectric Sensors Pyroelectric Sensors PE C Series Sensors 1 3 6 REAALKOOL Beam Splitter Assembly Beam splitter installed reflected beam on sensor Beam Splitter removed direct beam on sensor F S Beam Splitter 2 sided reflection unpolarized light 14 Beam Splitter Specifications y 1 Material UV grade fused silica go Spectral range 0 19 2 2um E Aperture 60mm E Damage threshold for pulses lt 10ns PW gt 300us PW S 5J cm gt 200J cm a2 Fraction split off See graph 0 200 400 600 800 1000 1200 1400 1600 1800 2000 2200 2400 2600 2800 3000 Wavelength nm Accessory Description Part number Heat Sink Heat sink that screws onto rear of PE25 and PESO series 7Z08267 sensors and allows working at over 50 higher average powers Scope Adapter Plugs in between the PE sensor and power meter 1Z11012 Provides BNC ou
62. File Path Name Delimiter Update Rate M2 Rail Setup Com Port and Length Connect Disconnect Rail Control ji Views Profiles Displays Beam Profiles for each axis with optional Gaussian m Overlays Results Displays Values and Statistics for Selected results Pointing Displays the XY position of the Centroid or Peak for each ROI with optional overlays and Accumulate Mode f Charts Displays Time Charts for User selected results 2D 3D Displays pseudo 2D 3D Beam Profile M Wizard An interactive procedure for measuring M2 by the Rayleigh Method File Saving NanoScan Data Files Text Files 8 Data Logging Log to File Reports NanoScan Report Automation Interface ActiveX Automation Server Minimum System Requirements PC computer running windows7 32 64 Laptop or Desktop Core CPU 2GHz or better 3GB of RAM or better 1 USB 2 0 port At least 250MB free HDD space 1440x900 Display Resolution or greater Add in PCI PCI Express graphics card w hardware acceleration DVD ROM drive Download the NanoScan Acquisition and Analysis Software Manual for a complete description of all Software Features VU OPHIR Photonics A Newport Corporation Brand Ga Corporation Brand For latest updates please visit our website www ophiropt com photonics Photon OPHIR Photonics A Newport Corporation Brand Ordering Information NanoScan Systems Both STD amp PRO NanoScan Systems Include Na
63. Finder In order to find compatible PC interfaces click PC Interfaces N NW a H NW lt 6 To save the results click Save To print the results click Print N Ee Sensor Finder Output Screen Y Another Search e Results For Energy Range 1mJ to 10 mJ Diameter 35 mm Rep Rate 10 Hz Wavelength 1064 nm Pulse Width 7 ns Name of Damage Threshold PDF 1 PESO lt 10 Th 2 PESOBF lt 10 L 3 PE50 DIF ER dif out lt 10 LE 4 PE50 beam splitter lt 10 LE 5 PE50BF beam splitter lt 10 Fi To download offline Sensor Finder version please click here To find a meter that connects to the sensor please click Meter Finder To find PC Interfaces that connects to the sensor please click PC Interfaces For further assistance contact us If sensor finder does not work properly please consult with your IT manager to reset the browser setting eg allow javascript Damage Threshold Some sensors are closer to the laser damage threshold than others Since the damage threshold can vary somewhat from case to case and also is cumulative the Sensor Finder Program mentions how close a particular sensor is to the damage threshold The displayed percent of damage threshold is the highest of either the power or the energy threshold It is recommended to select a sensor that is less than 50 of the damage threshold Power Energy Meters In order to find power energy meters or PC interfac
64. For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand Pyroelectric Sensors Pyroelectric type sensors are useful for measuring the energy of repetitively pulsed lasers at up to 25 000HZ and are sensitive to low energies They are less durable than thermal types and therefore should not be used Heat sink disc whenever it is not necessary to measure the energy of each pulse and average power measurement is sufficient Pyroelectric sensors use a pyroelectric crystal that generates an electric charge proportional to the heat absorbed Since the two surfaces of the crystal are metalized the total charge generated is collected and therefore the response is not dependent on beam size or position This charge then charges a capacitor in parallel with the crystal and the voltage difference thus generated is proportional to the pulse energy After the energy is read by the electronic circuit the charge on the crystal is discharged to be ready for the next pulse Pyroelectric crystal thickness lt Imm t etetetetttA t Electrical leads 1 0 SENLON Photodiode Sensors for Lower Powers In addition to the thermal sensors described above Photodiode sensors ieee are used for low powers from picowatts up to hundreds of milliwatts and Optical filter as high as 3W Photodiode A photodiode sensor is a semiconductor device that produces a current proportiona
65. Laser Laser pulse pulse pulse gt gt gt gt E 3 gt gt _ gt gt gt Depth of light penetration 0 1 1um Light Light is absorbed gradually over thick Depth of light Heat flows into and heat concentrated same thin layer Heat partially transmitting layer Heat is therefore ponei auon substrate during does not have a chance to flow during the generated over large volume even during 0 1 1uMm laser pulse short laser pulse duration short pulse with no heat flow Surface absorbers work best when measuring power or energy for long laser pulses A Volume absorbers can measure pulses with much higher energies than surface absorbers B C can measure Calibration Method and Estimated Accuracy for Ophir High Power Sensors Ophir models 5000W 10K W and Comet 10K are calibrated using relatively low power lasers 150 300W Using such low power lasers to calibrate the instrument vs the high power at which the sensors are used raises the question of calibration accuracy The following explanation clearly demonstrates that the 5000W 10K W and Comet 10K are indeed accurate to 5 over their measurement range The 5000W and 10K W sensors work on the thermopile principle where the radial heat flow in the absorber disk causes a temperature difference between the hot and cold junctions of the thermopile which in turn causes a voltage difference across the thermopile Since the instrument is
66. NanoScan 2 scanning slit profilers provide major enhancements to the ease of use and flexibility that customers have come to expect with its predecessors the world renowned NanoScan and BeamScan Capabilities NanoScan 2 is a PC based instrument for the measurement and analysis of optical beam spatial profiles in accordance with ISO standards Beam profiles are measured using the International Standard ISO 11146 Scanheads can also measure power in accordance with ISO 13694 NanoScan uses moving slits one of the ISO Standard scanning aperture techniques Measurement is possible for beam sizes from microns to centimeters at beam powers from microwatts to over kilowatts often without attenuation Detector options silicon or germanium allow measurement at wavelengths from the ultraviolet to the infrared The NanoScan2 digital controller has 16 bit digitization of the signal for enhanced dynamic range up to 220D ga optical With the accuracy and stability of the beam profile measurement you can measure beam size and beam pointing with a 3 sigma precision of several hundred nanometers The software controllable scan speed and a peak connect algorithm allows the measurement of pulsed and pulse width modulated lasers with frequencies of 20kHz and higher The ability to alter the drum speed also helps to increase the dynamic range allowing a much larger operating space for any given scan head see operating space charts for a graphic explanati
67. PD300R PD300R 3W PD300R UV 19 2 10 1 035 40 1 035 40 ui ADJUSTABLE LC SMU 76 125 J p 100 75 with filter off Q OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand with filter installed PD300R UV Lowest powers from 200 1100nm silicon o10mm Filter in Filter out Filter in 430 1100 200 1100 220 1100 3W to 200uW 3mW to 20pW 300mW to 2uW 3W to 30mW 3mW to 3nW 300mW to and dBm and dBm 300UW and dBm NA 0 001 100 mW nm mW mW 3000 250 350 3 300 3000 400 3 300 2000 600 3 300 1200 800 950 2 5 150 1200 1064 3 30 2200 NA 6 200 270 10 220 400 5 430 950 3 270 950 5 400 950 7 950 1100 5 950 1100 7 950 1100 100 10 50 500 0 4 15 l 0 2 3 2 SC ST FC SMA 7Z02438 PD300R IR 1 035 40 SM1 35 100 with filter off For latest updates please visit our website www ophiropt com photonics N Yi O N a9 LU N PD300R IR IR wavelengths 700 1800nm dg germanium q oomm Filter out Filter in 700 1800 700 1800 30mW to 5nW 300mW to 200uW 30mW to 30nW 300mW to and dBm 30mW and dBm 0 01 NA nm mW mW 800 12 120 1000 30 300 1300 1400 30 250 1500 25 80 1600 30 100 1800 30 300 5 700 900 7 700 900 4 900 1700 6 900 1700 7 1700 1800 9 1700 1800 10 50 0 3 3 200 0 2 2 SC ST FC SMA 7Z02439 24 2 1 035 40 ADJUSTABLE Ewi 76 125 l l 75
68. PE10 C 7202932 66 PE10 C StarLink 787152 66 75 PE10 S Consult Ophir representative 81 PE10 S Q Consult Ophir representative 81 PE25 A DIF XXX YYY Consult Ophir representative 82 PE25BB S Consult Ophir representative 82 PE25BB S DIF Consult Ophir representative 82 PE25BF C 7202935 67 PE25BF C StarLink 787154 67 75 PE25BF DIF C 7Z02941 69 Joa R 21 7 OU OPHIR Spiricon Photon Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics OPHIR Photonics 01 08 2013 Product P N Page PE25 C 7202937 67 PE25 C StarLink 787156 67 75 PE25 S Consult Ophir representative 82 PESOBB DIF C 7Z02947 70 PE50BB S Consult Ophir representative 82 PE5OBF C 7202934 68 PE5OBF C StarLink 78 153 68 75 PESOBF DIF C 7Z02940 70 PE50BF DIF C StarLink 78 158 70 75 PE50BF DIFH C 7 Z02943 70 PE50 C 7202936 68 PE50 C StarLink 78 155 68 75 PE50 DIF C 7202939 69 PE50 DIF C StarLink 787157 69 75 PE50 DIF ER C 7Z02948 72 PE50 S Consult Ophir representative 82 PE100BF DIF C 7202942 72 PE C to PE Size Adapter 7208273 Ti PFSA PHOOO052 167 PO PH00213 210 Pulsar 1 7Z01203 87 102 Pulsar 2 7Z01202 87 102 Pulsar 4 7201201 87 102 Pulsed InGaAs Option PH00185 208 Pulsed InGaAs Upgrade Option PH00186 208 PY III C A SP90092 154 PY III C B SP90093 154 PY III P A SP90090 154 PY I I P B SP90091 154 PY III W BK7 1 064 SP9010
69. PE25BB S DIF As above with diffuser for high damage 20mm 0 4 3um 3m4J 10J 30W 20Hz 50 8x18mm_ 82 threshold PE25 A DIF Compact high power built in electronics 824mm 0 4 3uMm 0 1mJ 10J 50W 1000Hz O50 8x28mm 82 XXX YYY PE50 S Slim profile large aperture no amplifier 846mm 0 19 3um 1mJ 10J 20W 10Hz 75x14mm 83 PE50BB S As above broadband coating O46mm 0 19 20um 10mJ 10J 15W 10Hz O75x14mm_ 83 Other Ophir offers many other OEM sensors For your OEM solution please fill the questionnaire on our website 84 Sensors www ophiropt com photonics or contact us USA sales ophir spiricon com Other ophir sales ophiropt com customer support ophiropt com Note a XXX denotes the calibration wavelength in um and the YYY denotes the calibrated sensitivity in V J 12 OU OPHIR 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand Sensor Finder Program Finding the proper sensor s to meet your measurement needs has never been easier With our sensor finder program just enter your laser parameters and the proper measuring sensors for your application will be displayed on the screen The program calculates the power and energy density capabilities of each absorber based on the laser wavelength pulse length repetition rate and other relevant parameters It also compares all the other requirements such as maximum and minimum power energy beam size etc
70. PHO0092 LENS 100 VIS Optional 100 mm focal length lens for use 400 700nm wavelength PHO0093 lt a LENS 100 NIR Optional 100 mm focal length lens for use 650 1000 nm wavelength PHO0094 LENS 100 LIR Optional 100 mm focal length lens for use 1000 1550nm wavelength PHO0095 1740 LENS MNT Lens mount for users wanting to use their own 25mm diameter lens PH00075 CUSTOM LENS Specify wavelength focal length PH00088 oD Model 1740 ModeScan Rail w o scan head PH00074 aa 1740 LENS PREP ModeScan custom lens PH00076 1740 TRNG ModeScan onsite operation training PH00077 CN Lens 400 2um Optional 400mm focal length lens for use at 2um wavelength PH00224 8 Lens 200mm VIS Optional 200mm focal length lens for use 400 700nm wavelength PH0O0237 o Lens 400mm VIS Optional 400mm focal length lens for use 400 700nm wavelength PH00238 M Lens 200mm NIR Optional 200mm focal length lens for use 650 1000nm wavelength PH00239 Lens 400mm NIR Optional 400mm focal length lens for use at 650 1000nm wavelength PH00240 Lens 200mm LIR Optional 200mm focal length lens for use at 1000 1550nm wavelength PH00241 lens 400mm LIR Optional 400mm focal length lens for use at 1000 1550nm wavelength PH00242 1 Q OPHIR Photon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand 3 7 Integrated Laser Performance Measurements 3 7 1
71. Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand A N D 40 lt 49 a9 aa L mM M 163 Photon OPHIR Photonics 01 08 2013 A Newport Corporation Brand 3 3 1 ERMEE 164 01 08 2013 NanoScan Acquisition and Analysis Software Feature NanoScan Standard NanoScan Professional all features in Standard plus Controls Source ScanHead Select Gain Filter Sampling Resolution i AutoFind Rotation Frequency Record Mode Capture Averaging Rotation Magnification CW or Pulse Modes Divergence Gaussian Fit Reference Position Recompute Regions of Interest ROI Single or Multiple Automatic or Manual Colors Profiles Vertical Scale 17 10 100 Logarithmic Scale Z amp PAN Automatic or Manual Computation ISO 13694 ISO 11146 Dat 13 5 50 2 User Selectable Clip Levels D46 Width ratios Centroid Position Peak Position Centroid Separation Peak Separation Irradiance Gaussian Fit Ellipticity e Divergence Total Power Pulse Frequency power Continuous Rolling Finite Pointing Centroid or Peak Accumulate Mode Beam Indicator Graph Center Colors 2D 3D 2D or 3D Mode Linear or Logarithmic Scale Resolution Fill Contours Solid Surface or Wireframe Clip Level Colors Charts Chart Select Parameter Select Aperture Select Update Rate Start and Clear Logging
72. Power Water Cooled Thermal Sensors and Power Pucks 1W 10kW 38 1 1 3 StarLink Direct to PC Power Sensors 42 1 1 4 Power Sensor Accessories 43 1 1 4 1 Accessories for PD300 Sensors 43 1 1 4 2 Accessories for Thermal Sensors PD300R PD300 IRG 3A IS FPS 1 44 1 143 High Power Water Cooled and Fan Cooled Laser Beam Dumps up to 10kW 45 1 1 5 OEM Thermal Sensors 46 Thermal OEM Sensors Introduction 47 1 1 5 1 Standard OEM Thermal Sensors 20mW 300W 49 Liss Examples of Custom OEM Power Sensor Solutions 54 1 2 BeamTrack Power Position Size Sensors Introduction 55 lad BeamTrack Power Position Size Sensors 100uUW 10W 56 lad BeamTrack Power Position Size Sensors 40mW 150W 37 EE BeamTrack Power Position Size Sensors 150mW 250W 58 1 2 4 BeamTrack Power Position Size Sensors Device Software Support 59 1 3 Energy Sensors 61 Energy Sensors Introduction 62 Absorption and Damage Graphs for Pyroelectric Sensors 63 Wavelength Range and Repetition Rate for Energy Sensors 64 Fe Photodiode Energy Sensors 10pJ 20uJ 65 LZ Pyroelectric Energy Sensors 0 2uJ 10J 66 EE High Energy Pyroelectric Sensors 20uJ 40J 69 1 3 4 RP Sensors 100mW to 1500W 73 Ee StarLink Direct to PC Energy Sensors 75 1 3 6 Energy Sensors Accessories 76 130 1 Accessories for pyroelectric sensors 76 1 3 6 2 Fast Photodetector Model FPS 1 78 1 3 7 OEM Energy Sensors 79 Standart Pyroelectric OEM Sensors Introduction 80 EF Standart OEM Pyroelectric Energy Sensors 2uJ 10J 81 Err Examples of Custom O
73. Spectral Range um 0 19 20 0 19 20 0 19 20 Aperture mm p26 p26 p26 Power Mode Maximum power 10W free standing 50W heat sinked 10W free standing 50W heat sinked 10W free standing 50W heat sinked Minimum power 80mW 80mW 80mW Power Noise Level 4mW 4mW 4mW Maximum Average Power Density kW cm 17 at SOW 28 at 10W 17 at SOW 28 at 10W 17 at 50W 28 at 10W Response Time 0 95 typ sec 1 5 1 5 1 5 Power Accuracy at calibrated wavelength 3 J J Linearity with Power 1 1 1 Amplifier power supply for UA UAU versions NA 6V to 24V Via host USB Energy Mode Maximum Energy 30J 100J 100J Minimum Energy 30m4J 30m4J 30mJ Energy Accuracy at calibrated wavelength 5 5 5 Maximum Energy Density J cm lt 100ns 0 3 0 3 0 3 0 5ms 5 5 5 2Ms 10 10 10 10ms 30 30 30 Cooling conduction conduction conduction Output Ophir smart plug 6 pin Molex Mini B USB connector Dimensions 60x60x38mmM 60x60x38mmM 60x60x38mmM Part number 773434 Consult Ophir representative Consult Ophir representative Note a With analog UA version maximum power is also limited by maximum output voltage where output voltage is at most 2V less than input voltage Note b 4 pin Molex connections Voltage Voltage Analog signal out Ground 6 pin Molex connections RS232 input Ground Voltage Analog signal out high low voltage or switch input when used RS232 output Note c Calibrated at customer selected wavelength L30C SH L30C UA 38 60 2x M3x5deep
74. Wireframe Clip Level Colors Charts Chart Select Parameter Select Aperture Select Update Rate Start and Clear i Logging File Path Name Delimiter Update Rate M2 Rail Setup Com Port and Length Connect Disconnect Rail Control i Views Profiles Displays Beam Profiles for each axis with optional Gaussian N o Overlays E E _ Results Displays Values and Statistics for Selected results soe Pointing Displays the XY position of the Centroid or Peak for each zas ROI with optional overlays and Accumulate Mode Charts Displays Time Charts for User selected results 2D 3D Displays pseudo 2D 3D Beam Profile ag M Wizard An interactive procedure for measuring M2 by the Rayleigh Method C File Saving NanoScan Data Files ab Text Files mM Data Logging Log to File e Reports O NanoScan Report O M Automation Interface ActiveX Automation Server Minimum System Requirements PC computer running windows 7 32 64 Laptop or Desktop i A dual core processor CPU 2GHz or better 2GB of RAM 1 USB 2 0 port available At least 250MB of free HDD space 1400 x 900 display resolution or better Graphics card w hardware accelerator DVD ROM drive 7 Microsoft compatible pointing devices e g mouse trackball etc Download the NanoScan Acquisition and Analysis Software Manual for a complete description of all Software Features 1 A business professional version of windows is recommended The NanoScan v2 software has not been tes
75. With the Laserstar Pulsar USBI Quasar and Nova or Orion with adapter only 2 of the 5 pulse width settings are available For the PE C models the 30us and 1ms settings and for the PE BF models the 1ms and 10ms settings Note f The 3000nm setting is calibrated for 10 6um as well To measure CO laser set to the 3000nm setting The additional error for measuring 10 6um is 5 For sensors drawings please see page 71 Q OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand 1 3 2 Wialaselss 68 01 08 2013 1 3 2 Pyroelectric Energy Sensors 10pJ to 10J PE50 C PESOBF C Energy Sensor with Features optional heat sink 46mm apertures Metallic coating for high rep rates BF coating for highest damage threshold Rep rates up to 10kHz Measure lasers with pulse widths up to 20ms New compact PE C series Model PE50 C PESOBF C Use High rep rate High damage threshold Aperture mm p46 p46 Absorber Type metallic BF Spectral Range um ve 015731060 Surface Reflectivity approx 50 20 Calibration Accuracy 3 3 Max Pulse Width Setting 2us 30us 500us Ims 5ms Ims 2ms 5ms 10ms 20ms E Sed 10J to 10J to 10J to 10J to 10J to 10J to 10 to 10J to 10 to 10 to fei deo 200W 200 2m 2m am mm 20m 20m 20m Lowest Measurable Energy uJ 69 10 10 60 80 100 120 300 600 600 600 Max Pulse Width ms 0 002 0 03 0 5 1 5 1 2 5 10 20 Maximum Puls
76. Y OPHIR Spiricon Photonics For latest updates please visit our website www ophiropt com photonics Soy eee ES 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand 3 4 7 Uxeeiaawalariais 182 01 08 2013 UView Ultraviolet Converter for C mount Cameras The UView accessory converts ultraviolet radiation into a visible green beam profile that is reimaged onto a CCD style C mount camera The UView operates over the ultraviolet region of 190 390nm It has a reimaging magnification factor of 0 5x and a field of view FOV of 15x20mm with an SP620 style camera The FOV will vary with camera format Camera and software sold separately UView top view UView with camera sold separately 4 017 r al CL TX 420 UNC 26 F 127010500 UView Image Converter specifications Specifications Beam redactions 0 50X nominal image reduction Scale factor 2 0 nominal scale factor for BeamGage see label Spectral range 190 to 390nm Minimum signal 1uJ cm Camera saturation 30mJ cm at 193nm 15mJ cm at248nm Varies with wavelength and camera type Clear apreture 18mm X 22mm Effective apretute 15mm X 20mm w SP620 varies with camera format Damage threshhold 5W cm 100mJ cm Mounting 3 1 4 20 threaded mounting points see figure 11 Dimensions see figure 7 Weight Xxx OZ yyy g w o camera Adaptable beam analyzer The Uview can be used with the following cameras
77. a thermopile voltage generating device it must be linear at low values of output Therefore if it is shown to be linear at powers which are a significant fraction of the maximum power it will necessarily 2 OPHIR a For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand rt Corporatio 1 1 Qtetatsreras 01 ao 2 o HIR be linear at very low powers and if the calibration is correct at low powers it will remain correct at high powers as well On the other hand although the output may be linear at low powers there may be a zero offset that due to the relatively low output at low powers will cause an error in calibration For example if calibration is performed at 200W and the output of the sensor is 10uV W a typical value and there is a zero offset of only 1uV this will cause a calibration error of 10 Ophir s calibration method always measures the difference between the reading with power applied and without power applied thus eliminating error due to zero offset This measurement is taken several times to insure accuracy The above measurement method assures that the calibration inaccuracy due to measurement errors is less than 1 comparable to the expected errors in our lower powered sensors In order to verify this models L1500W 5000W and 10K W sensors have been measured by various standards laboratories These measurements have shown Ophir sensors to be well wit
78. absorber Spectral Range um 0 19 20 0 4 1 5 10 6 0 8 2 10 6 Aperture mm p 50mm p 50mm 045mm Power Mode Power Range 20W 5000W 20W 5000W 100W 10kW Power Scales 5000W 500W 5000W 500W 10kW 1kW Power Noise Level 1W 1W 2W Maximum Average Power Density kW cm 6 at 1000W 3 at 5000W 7 at 1000W 4 at 5000W See note below Response Time with Meter 0 95 typ s 2 3 2 7 Power Accuracy 5 50 5 Linearity with Power 2 2 2 Energy Mode Energy Range NA NA NA Energy Scales NA NA NA Minimum Energy mJ NA NA NA Maximum Energy Density J cm See note below lt 100ns 0 3 0 05 Tus 0 4 0 3 0 5ms 5 20 2MS 10 50 10ms 30 150 Cooling water water water Minimum Water Flow Rate at Full Power 4 5 liter min 4 5 liter min 9 liter min Weight kg 2 8 2 8 4 5 Version V1 Part number 7Z02119 7Z02255 7Z02645 Notes a Calibrated for 0 8um 1 064um and Calibrated for 1 064um and 10 6um Calibrated for 1 064um and 10 6um 10 6um Notes b vet temperature range 18 30 C Water temperature rate of change lt 1 C min Notes c Beam diameter Max power density Max energy density 1ms pulse width 3ms pulse width 10ms pulse width lt 15mm 10kW cm 30J cm 60J cm 150J cm 15 20mm 7kW cm 20J cm 40J cm 100J cm 20 40mm 5kW cm 15J cm 30J cm 70J cm 40 45MM 4kW cm 12J cm 25J cm 60J cm 5000W 5000W LP m 10K W e eee 2146 146 2x 1 8 NPT 045 READ SIZE 34 5 pee 27 Q
79. adjust your laser resonator and beam delivery optical system for optimum beam quality on line You can also measure the cross section at any point as shown The illustration shows the intensity distribution of a pulsed Nd YAG laser where the X and Y profiles are taken at the cursor lines which can be placed anywhere on the beam This data can be saved brought back and manipulated at any time so you can compare the present profile with a reference The system has an exclusive optical design making it easy for you to adjust the intensity to get the optimum picture by just pushing and pulling the attenuating filter adjustment levers The beam profile can also be shown in a three dimensional form which can be rotated to different angles and elevations Coenen oa a ee fK fj i aK aaa DOE EE i puii i i it 1E T i ii tal HH E i i i an tit bead ak taal Temporal Pulse Shape The temporal profile of laser pulses important in obtaining consistent process results can now be easily monitored Shown to the right is the pulse shape of the same pulsed Nd YAG laser with 2ms pulses It is being measured with a PC oscilloscope available as an accessory You can display the pulse shape alone or together with the beam profile on your PC Plug the Beam Cube output into an oscilloscope to observe the temporal pulse shape of your laser beam wee ST cei iiit i 3 7 1 UxSeiaawa
80. and a moving lens If the laser beam is diverging or converging within the travel range of a moving lens the reported M value and other results can be significantly compromised Spiricon s M 200s Beam Propagation Analyzer is fully ISO 11146 compliant Automatic M2 at Production Speeds The M 200s optical train uses a fixed position lens and camera The mirrors that direct the focused beam into the camera are moved to precise locations translating the beam through both the waist region and the far field regions All these measurements and translations as well as incremental beam attenuation are automatically controlled by the M 200s software Software improvements in the M 200s including more efficient algorithm execution has decreased the measurement reporting time by 2 3 times making it possible to report M in under two minutes Steering Mirrors Beam Attenuater Laser Source Camera m 200s Alignment Tool Optical Train OU OPHIR Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand A VA D GD lt L 40 WU aa O aa 187 i ee OPHIR RAELE 01 08 2013 A Newport Corporation Brand ewport Corpor Manual M2 Manual mode is available for beams that are too large or too small or at wavelengths outside the standard optical train Accuracy by Design Spiricon products are known for accuracy Using our pate
81. and cabling or any options for safe storage in an industrial facility Weight 8 Ibs 3 6kg Beam Dump optional Power Meter optional Laptop Computer Compliance Water cooled and rated for 5kW total power 5000W SH up to 5kW total power 10kW SH V2 up to 10kW total power Provided by user Vista 32 or Windows 7 is required Unit meets CE and RoHS requirements Sampling Wand 5000 Sampling Wand 4750 4500 4250 4000 3750 3500 3250 3000 2750 2500 2250 2000 Beam Power in Watts 1750 Beam Power in Watts 1500 1250 1000 750 500 250 0 5 10 15 20 25 30 35 40 0 5 10 15 20 25 30 35 40 Beam Diameter in mm Damage and Saturation Power vs Beam Dia Beam Diameter in mm Damage and Saturation Power vs Beam Dia Safe Operation is to the Right of the Solid line Image Saturation is approximately the Dashed line Chose a sampling Wand that 3 B 0 Uxeelaawatarciiasis contains your beams maximum power and minimum diameter to be near but below the dashed line for safe and best beam viewing Ordering Information Item Description P N MODECHECK CO 5kW ModeCheck CO sampler for 10 6um beams up to 5kW beam width up to 30mm includes 2 user SP90211 selectable wands from selection below 0 5 wa
82. and positioned simultaneously Cartridge inserts into the 1D Cartridge FFC Fiber Cleaver for use with the Photon Fiber Clip PH00203 REF Standard reference cartridge Includes a Photon Standard SMF 28 Reference Cartridge and a 1310nm OdBm LD PH00204 Light Source BFC Bare fiber connector for LD8900HDR Cartridge has a v groove and clamp for holding fiber Fiber is positioned PH00205 manually to a visual reference position Intended for use with specialty fibers that canno 3D 3 D scan module for HDR Interchangeable accessory adds full 3 dimensional measurement capability with up to 200 PH00206 cuts through the fiber Includes a 3D Scan Module and Motion Controller CFP Connectorized fiber mount for HDR Adapter plate for mounting connectorized fibers Standard ST FC and SC PH00208 connectors are held by the ferrule tip Call for other types Case Rugged shipping case for LD8900HDR PH0O0209 MfgSoft Software interface designed for manufacturing Simple interface screen shows the high dynamic range 1D profileand PH00210 reports MFD Aeff and NA Includes fields for time stamps serial numbers and notes 1W Mount 1 D waveguide mount Waveguide mount for use with 1D Interface Plate PH00215 3W Mount 3 D waveguide mount Waveguide mount for use with 3D Scan Accessory PH00216 1CustomFxt Custom mnt for 1 D vers of HDR LED Prof Custom designed fixtures for mounting novel sources for 1D scans PH00217 LED Profiler A goniometric profiler designed to rapidly measur
83. available from 13 to 355 nm and 1 06 to gt 3000 um m Image CO lasers telecom NIR lasers and other infrared sources out to Far IR THz sources m Solid state array camera with 1000 1 linear dynamic range for accurate profiling m Integrated chopper for CW beams and thermal imaging m Versatile Firewire interface all res ieii e EEn Interchangeable windows available for a variety of i applications i m mage Viewer utility presents 3D isometric plots 2D color ws maas TIT T T OSLA LE l Rir iH contour plots and grayscale among other views girim m Includes BeamGage Laser Beam Analysis Software for extensive aratma quantitative analysis and image display Spiricon has been the world leader in the manufacture of pyroelectric solid state detector arrays and cameras For over 25 years the Pyrocam has been the overwhelming camera of choice for Laser Beam Diagnostics of IR and UV lasers and high temperature thermal imaging Precision stability reliability and versatility have become its proud heritage The Pyrocam Ill offers easy Windows camera setup direct Windows quantitative and image display 14 bit digitizer versatile Firewire PC interface an integral chopper for CW beams and thermal imaging and many other enhanced features See Your Beam As Never Before The Pyrocam III camera creates clear and illuminating images of your laser beam profile Displayed in 2D or 3D views you can immediat
84. cameras with pulses Comes with a BNC cable Stand for mounting sold separately Dual beam splitters and configurable 9 ND filters for 190 1550nm screws onto front of camera OU OPHIR Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand P Spiricon OPHIR Photonics 01 08 2013 P N SP90279 A SP90280 D SP90281 a0 SP90282 lt SP90219 D SP90229 aa SP90230 N SPZ17005 gt CY SP90186 139 A Newport Corporation Brand Newport Corporation Brand 3 2 3 Cameras 3 2 3 1 190 1100nm USB Silicon CCD Cameras SP Series Features USB 2 0 compatible m 64dB true system dynamic range highest in the industry m Programmable high speed electronic shutter m Spectral range 190 1100nm m Gain adjustable to accommodate a wide range of input levels m Built in optical trigger synchronizes with even the shortest laser pulses Slim profile and multiple mounting options Built in photodiode trigger SP503U SP620U L Series Features m 35mm format for large beams m 59dB true system dynamic range m Spectral range 190 1100nm USB L11059 ACTIVE AREA 3 2 3 1 Ween Walerclals IMAGE AREA F 35mm A 24 mm 2 Q O
85. coated from 400 700nm This diagram shows the 6mm offset of the through beam that is created by the reflecting optic The deflection angle of the output beam is less than 0 007 degrees The rear surface of the flat is AR coated to maximize the throughput of the main beam The standard Beam Tap II rear surface is AR coated for 400nm 700nm The YAG version is AR coated for 1064nm on both surfaces 6mm Typical Beam Offset Beam tap relection vs wavelength Shown is the Beam Tap II final sampled reflection vs wavelength As shown both the S amp P reflection are nearly constant at 0 05 from the UV to the infrared Ordering Information Model Surface Wavelength range Optical Material Reflection P N BT I Single surface 1 cube 400 700nm UVFS 4 Ravg SP90135 BT ll Dual surface 2 cubes 400 700nm UVFS 0 16 Ravg SP90133 BT I YAG Single surface 1 cube 1064nm BK7 0 5 Ravg SP90173 BT II YAG Dual surface 2 cubes 1064nm BK7 0 0025 Ravg SP901 72 Stackable Beam Splitters The stackable beam splitters are designed for maximum modularity and shortest beam path They are compatible with almost all of our cameras having the standard C mount thread and can mount either to other attenuators or to the camera itself Each beam splitter reduces the intensity of the beam by 20 times see graph below so if a camera is equipped with filters that can operate with lasers typically up to 1 Watt with one beam splitter it can Operate up to 20 Watts
86. employed by BeamGage LBA and BeamStar products This product camera systems will work with any X CS mountcamera but the FOV will vary based on imager format SP503 SP260 SCOR20 GRAS20 FASO FA33 FX33AD L070 L130 L230 1 The UV converter glass will damage before it becomes saturated Ordering Information Item Description P N UView Uview Accessory for C mnt Cameras SP90322 VO OPHIR Spiricon Potoni For latest updates please visit our website www ophiropt com photonics OPR emonies A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand 3 5 Near Field Profilers 3 5 1 Camera Based Near Field Profiler Allows measurement of beams normally too small for camera profiler Expands beam to reduce power energy density Provides near field profile of fibers LD junctions and other small sources Can be used to measure tightly focused beam with camera and attenuation Nominal 10X 20X 40X 60X Beam expansion available Easily calibrated to provide absolute measurement values Built in continuously variable attenuation C mount for attachment to any camera profiler Camera and BeamGage software purchased separately Near field profiling can also be used with camera profilers to analyze small beams and involves a microscope objective lens to image the beam onto a camera detector array This technique expands the measurement range of the camera to include smaller beams which could not be ordina
87. error at 193nm 46 Max additional error at other wavelengths not specified above 3 193nm reading may need 1min irradiation to stabilize At other wavelengths there may be an additional error up to the value given For wavelengths gt 2um derate to 10 of above values For wavelengths below 600nm derate to 60 of given values for DIFH 50 of given values For wavelengths below 240nm derate to 1J cm For beam size lt 5mm For 10mm beam derate to 50 of above values Notes b Notes c With the user threshold setting set to minimum For other settings the spec is for gt 7 of full scale or greater than twice the user threshold whichever is greater The user threshold is available with Nova Il Vega StarLite or Juno For other meters the threshold is set to minimum and the linearity spec is gt 10 of full scale The PE C series will only operate with Nova or Orion meters with an additional adapter Ophir P N 7Z08272 see page 77 The adapter can introduce up to 1 additional measurement error The user threshold feature allows adjustment of the internal threshold up to 25 of full scale if desired to avoid false triggering in noisy environments The user threshold setting represents the approximate minimum energy for pulse widths below 50 of the pulse width setting For longer pulse widths the actual minimum may be higher For highest accuracy it is recommended to zero the sensor against the meter the first time it
88. exposure times running CW at 632 8nm wavelength Camera set to minimum useful gain for saturation test and maximum useful gain for lowest signal test 2 The maximum rate depends on the RO Region of Interest size the bits readout and the number of cameras on the same bus The SCOR 20 operates at 7 5Hz 12 bits and 15Hz 8 bits It operates up to at least 60Hz with a smaller ROI The frame rate also depends on PC resources 3 May be usable for wavelengths below 350nm but sensitivity is low and detector deterioration may occur Therefore UV image converter is recommended Although our silicon cameras have shown response out to 1320nm it can cause significant blooming which could lead to significant errors of beam width measurement We would suggest our XC130 InGaAs camera for these wavelengths to give you the best measurements 4 This is the damage threshold of the filter glass of the filters Assuming all filters mounted with ND1 red housing filter in the front Distortion of the beam may occur VU OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics 2 Spiricon OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand 3 2 3 3 190 1100nm Gig E Silicon CCD Cameras Models Gevicam Features m Ethernet compatible Oo m Long cable distances m High speed image acquisition E Gevicam 8 0 i
89. higher damage O35mm 0 19 2 2um 200 103 250Hz 70 threshold 2 94umM PE5OBB DIF C Pyroelectric with removable diffuser Wide spectral 046mm 0 19 20um 0 4 100uJ 40J 40Hz 70 range w o diffuser O33mm with 2 5um with diffuser diffuser PE50 DIF ER C Pyroelectric with removable diffuser Especially for 046mm 0 19 3um 0 4 3um 10uJ 30J 10 000Hz 72 Erbium laser O33mm with with diffuser diffuser PE100BF DIF C Largest aperture pyroelectric with removable diffuser 96mm 0 15 3um 0 4 400uJ 40J 200Hz 72 O85mm with 2 5um with diffuser diffuser RP sensors 200mW 1500W Sensor Features Aperture Spectral Range PowerRange Maximum Frequency Page FL250A RP Long pulse lasers to 250W O50mm 0 19 6um 200mMW 250W 15 000Hz 73 L1500W LP1 RP High power pulsed lasers O50mm 0 6 1 1um 10W 1500W 15 000Hz 73 OU OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand StarLink Direct to PC Energy Sensors Sensor Features Aperture Spectral Range Energy Range Maximum Frequency Page PE10 C StarLink Pyroelectric for low energies O12mm 0 15 12umM 1uJ 10mJ 25 000HZz 75 PE25 C StarLink Medium aperture pyroelectric O24mm 0 15 3yum 8uJ 10J 10 000Hz 75 PE25BF C StarLink As above high damage threshold O24mm 0 15 3um 10 6um 60uJ 10J 250Hz 15 PE50 C StarLink Large aperture pyroelectric O46mm 0 15 3um 10uJ 10J 10 000Hz 75 PESOBF C StarLink As above high damage threshold O46mm 0
90. is used with a particular meter For further information see the FAQs on our Website Notes d A shock absorbing mounting post is available for situations in which sensor is mounted on a surface subject to shock or vibration This can prevent false triggering and allow working at lower minimum energies Note however that in this case the maximum average power will be reduced to 13W without heat sink and 25W with heat sink see accessory pages 76 77 for heat sink and mounting post Notes e With the Laserstar Pulsar USBI Quasar and Nova Orion with adapter only 2 of the pulse width settings are available For the PE BF models the 1ms and 10ms settings and for the PE BB model the 3ms and 10ms settings For sensors drawings please see page 71 Q OPHIR Photonics A Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics PE25 C PE25BF C PE50 C PESOBF C 21 Tr 21 P46 p62 7 5 10 5 ADJUSTABLE 90 139 ADJUSTABLE 90 139 100 75 i 100 i 75 PE25BF DIF C 28 5 PE50BF DIF C PE50 DIF C 35 ADJUSTABLE 90 139 ADJUSTABLE 90 139 100 p 75 l 100 it 75 PE50BF DIFH C PE50BB DIF C m 33 Diffuser In 46 Diffuser Out 262 SSSI SSSSSE 4 BSS DOK Removable Diff
91. laser beam for profile measurements or for monitoring power or energy However as shown at 45 a single surface reflects the S polarization component at more than 10 times the reflection of the P component Depending on the laser polarization content or stability this sampling can provide very misleading and unreliable measurements The BT I YAG has both surfaces A R coated for 1064nm so the reflection for both polarizations is equal at 0 5 At other wavelengths far from 1064nm the above discussion applies Equalizing S amp P reflected polarization Any arbitrary polarization component can be broken into equivalent S amp P components With complimentary sampling surfaces any given component gets reflected once as the S polarization and the second time as the P polarization Thus using 2 surfaces the total reflected energy for all polarization components is the sum of the S reflectance and the P reflectance This causes the sampled beam to have S amp P components that are identical to the original beam 3 4 3 PERMENO Y OPHIR Y Spiricon Photonics For latest updates please visit our website www ophiropt com photonics Sy eee ES 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport A Newport Corporation Brand Brand Beam path through beam tap The Beam Tap Il uses two reflecting surfaces such that the two planes of reflection are orthogonal The standard Beam Tap rear surface is AR
92. measure it again 3 Compare the results 4 The Standard Deviation below is about 3 which is phenomenal compared to the 100 or more of any beam profiler without Ultracal LAr f i F i 2 irera D4oM 2 750e 02 Mean 2250e 02 StdDey 6 6270e 027 um T Dioni 2 3258407 Mean 7311 07 StdDbew 7 0932 00 um lab ary HLT alaa A Beam at full intensity Width 225um Std Dev 0 06um eam attenuated 100X displayed here in 2D at 16X ak zoom Width 231um Std Dev 7um Adding the use of Automatic Aperture improves the accuracy to 1 The conditions of this measurement is a camera with a 50dB SNR 5 You normally don t make measurements at such a low intensity But occasionally you may have a drop in intensity of your beam and don t want to have to adjust the attenuation Or you may occasionally have a very small beam of only a few tens of pixels In both of these cases Ultracal becomes essential in obtaining accurate measurements 3 2 1 1 Uxelaawatarelaiis 20 E Lt VO OPHIR Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Beam Measurements and Statistics BeamGage allows you to configure as many measurements as needed to support your work and comes standard with over 55 separate measurement choices To distinguish between calculations that are based on ISO standards and those that are not a graphical ISO logo i
93. min 2 5 liter min Weight kg 0 8 0 8 1 2 12 Version V2 V2 V1 V1 Part number Standard Sensor 7Z02664 7Z02668 7Z02661 7Z02665 StarLink Sensor Direct USB link to PC p 42 787005 Notes a Calibrated for 0 8um 1 064um Calibrated for 1 064um and Calibrated for 0 8um 1 064um Calibrated for 1 064um and and 10 6um 10 6um and 10 6um 10 6um Notes b Water temperature range 18 30 C Water temperature rate of change lt 1 C min 1000W 1000W LP L1500W L1500W LP 9120 20 1 8 NPT 1 8 NPT THREAD SIZE 21 5 THREAD SIZE ee L 15 30 ADJUSTABLE ADJUSTABLE 112 158 1 4 BSW 125 165 THREAD FOR ROD QUICK CONNECT FITTING FOR 2s a ASTIC HOSE FOR 3 8 PLASTIC HOSE l La 100 75 Q OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand 1 1 2 6 High Power Water Cooled Thermal Sensors and Power Pucks 100W to 30kW Features 30K W m Highest powers m Water cooled Up to 30kW ve o 4mm apertures O Y W N O Model 30K W N Use Highest powers to 30kW Absorber Type Beam deflector broadband absorber a Spectral Range um 0 8 2 10 6um Aperture mm 074mm Power Range 100W 30kW Power Scales 30kW 6kW 600W Power Noise Level 1W Backscattered Power Approximately 4 Maximum Average Power Density kW cm 10kW cm anywhere in the beam Response Time with Display 0 95 typ s 7S Powe
94. minimum frequency is a function of the beam size and the scan speed This is a simple arithmetic relationship there must be a sufficient number of pulses during the time that the slits sweep through the beam to generate a meaningful profile Please refer to Photon s Application Note Measuring Pulsed Beams with a Slit Based Profiler OU OPHIR Photon Potoni For latest updates please visit our website www ophiropt com photonics ORE Photonies A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand NanoScan Main Display Screen File Menu Quick Access Toolbar Panel Title Bar Ribbon Bar Standard Windows Controls Ribbon Tabs a FA MeO Lr a H f ami bee EA TS pL Pi Mee eet Pe N y Source Prk Pit ng piil impu ahin reser pia Par s ging Ka alyie LEA ree ih a Tanhead aii a 13 5 Wielth Al prj 13 5 Width 42 pen Detsigrs l um Dinga AZ ur Genkecud Perion Al urs Centroid Position AZ urn Peak Postion 4 um Peek Parten Az umn BAO 124241 Ah Results Window User Notes Status Bar Primary Dock Window note tabs The Most Versatile and Flexible Beam Profiling System Available 3 3 1 PEMEVE Photon s NanoScan scanning slit profilers provide major performance enhancements while maintaining the ease of use and flexibility that customers have come to expect with its predecessor the world renowned BeamScan NanoScan scanh
95. more with included StarLab application m LabVIEW VIs COM Object Interface and ActiveX software included a Smart Sensor to Pulsar to PC Ophir s 1 4 channel Pulsar interface turns your PC or laptop into 2 a full fledged Ophir multi channel laser power energy meter U Just install the software plug the sensor into the Pulsar and the D USB cable from the Pulsar to the PC USB port With the Pulsar series you can connect up to 4 sensors to each module monitor each pulse at up to 25kHz and utilize external trigger z ag Baki la Dee dae Dph Dp r i N Stee N n bed N LabVIEW Pulsar 4 operating with StarLab software Specifications Power Measurement Power log period 55 10 S00NK Energy Measurement Max real time datalogging toPC 25 000Hz Trigger input and output Timing General Number of sensors supported Compatible sensors Power supply Dimensions Notes Ordering Information BNC trigger input to enable measurement of missing pulses or to select specific pulses Can also be configured to give trigger output Supports time stamp for each pulse resolution 1us 4 2 11 sensors per unit Can combine several units with software for display of up to 8 sensors on one PC Supports all standard Ophir pyroelectric thermal and photodiode sensors 12V wall cube power supply plugs into jack on rear The power supply can be ordered from your local distributor 189 x 103 x 33MM a Limited by the maximum rep
96. of this market by providing measurement systems that have a high damage threshold and the ability to measure high repetition rates with high accuracy There are two main types of laser for industrial and material processing applications the CO laser at 10 6 microns and the Nd YAG laser at 1 064 micron These lasers are used for cutting welding trimming marking and other functions on many types of material such as metal wood plastic etc They are characterized by their high power output which ranges from ns le a at Ts set ITT j ii ff 100W to 30kW depending on the application With its capabilities in power energy and profile measurement Ophir has developed many products for this market including an integrated Laser Beam Analyzer for industrial YAG lasers which measures beam profile temporal profile power and energy all in one unit A subset of the industrial market is the microelectronics industry which uses excimer lasers for exposing the photoresist in the photolithography process This process uses lasers with a short wavelength of 193 to 345 nm that operate at high repetition rate and high energy The main factor influencing the component density possible on the microchip is the wavelength of the laser already used in the process and therefore the trend is to progress to shorter wavelengths Ophir has a range of unique products specified for the photolithography market including off the shelf and OEM prod
97. of trying to build a mechanical part without a micrometer So why attempt to build lasers or laser systems with only a power meter You will produce the desired results more quickly if you can measure basic things like beam width or size beam profile and power We believe as Lord Kelvin said You cannot improve it ifyou cannot measure it 3 1 1 Four Basic Questions When choosing a laser beam profiler there are a plethora of choices to do the job including CCD and CMOS cameras scanning slit sensors InGaAs and pyroelectric cameras pinhole and knife edge sensors to mention some How does one decide which is the proper solution for one s application and from which company to obtain the profiler system When making the selection there are four basic questions about the laser application that one must answer Wavelength ewe The first question is What wavelength s do you intend to measure 100 Diameter The answer to this question determines the type of detector needed Measured and what the most cost effective approach may be For the UV and erg visible wavelength range from lt 193nm up to the very near infrared Voltage at around 1300nm silicon detectors have the response to make these 50 measurements The largest number of cost effective solutions exist for these wavelengths including CCD cameras and silicon detector equipped scanning aperture systems Which of these is the best will be 13 5 determined by the answers t
98. only beam profiler on the market using modern Windows Vista and Windows 7 navigation tools The menu system of BeamGage is easy to learn and easy to use with most controls ay one mouse click away Some ribbon toolbar examples erm ocr corona i ae Bai S Thana ce ae imu m o unupa e on ee i S cma aha Ei JE HE on rare al Jalil Fm E oo e E Pol ee o a i iega a Relea Sige Feir Liha Hinin lirga atu fis Ph baue ie uf 4 4 Wi ath eg buns Hee ome i haem Soe ee Th et oe oe a ag uri m U n Some of the Beam Capture options Q OPHIR O Spiricon Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport A Newport Corporation Brand Brand BeamGage Main Display Screen Quick Access Toolbar Tabbed Control Tool Windows that dock User Definable Integrated Help for common tasks Access inside or float outside App Window Layout System n 2D Beam Display File Save Load ApplicationButton 6 8 7 wit een Chay Li a a mm mm bee 14 DnA Creat bil iremm Hop afar Pare Pri Simi LE a i a Coie ie E z jo biasae Fe Jrad Iii pal ca Wi 2 os Dimma 2 as F Moor Gace Power Eneigy a ier wt hes laja Gaini Halgi J LITRENI Birmoyrd Y feu Std T Description abue Mean Std Dev rit fs ai ta aa Total Pwr ISO 1 000e
99. output mini USB connection digital output only Features High power smart sensor High power built in High power built in amplifier amplifier water cooled Absorber Type Broadband Broadband Broadband Spectral Range um 0 19 20 0 19 20 0 19 20 Aperture mm 018 018 018 Power Mode Maximum power 60W if used with suitable 60W if used with suitable 150W heat sink 5W free standing heat sink 5W free standing Minimum power 60mW 60mW 100mW Power Noise Level 3mW 3mW 5mW Maximum Average Power Density 30at5W 20 at 60W 30 at 5W 20 at COW 12 at 150W kW cm Response Time 0 95 typ sec 1 2 1 2 1 2 Power Accuracy at calibration 3 3 a wavelength Linearity with Power 1 1 1 Amplifier power supply NA 6V to 24V 6V to 24V Via host USB for UA UAU versions Energy Mode where applicable Maximum Energy 100J 100J 100J Minimum Energy 20m4J 20m4J 50m4J Maximum Energy Density J cm lt 100ns 0 3 0 3 0 3 0 5ms 5 5 5 2Ms 10 10 10 10ms 30 30 30 Cooling Conduction Conduction Water Output Ophir smart plug 6 pin Molex 6 pin Molex Mini B USB connector Dimensions 50 8x50 8x33mmM 50x50x38mmM 50x50x38mm Part number 77023 Consult Ophir representative Consult Ophir representative Consult Ophir representative Note a With analog UA version maxim
100. photodiode sensors 7Z01560 Carrying Case Carrying case 38x30x11 cm For power meter and up to 3 sensors 1J02079 USB Cable for Vega USB to mini DIN cable 1 unit supplied with Vega 7E01205 RS232 Cable for Vega D9 to mini DIN cable 1 unit supplied with Vega 7E01206 Battery Pack for Vega Replacement battery pack for the Vega 7E14007 90 OU OPHIR 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 2 1 2 Nova ll Versatile Laser Power Energy Meter Compatible with all Ophir thermal BeamTrack pyroelectric and photodiode sensors Large high definition LCD display Choice of digital or analog needle display 2 position kickstand Backlighting and rechargeable battery Analog output Log every point at up to 4000HZ with pyro sensors Non volatile data storage up to 54 000 points Laser tuning screen and power and energy log USB and RS232 interfaces with StarLab and Starcom PC applications LabVIEW driver COM Object Interface and Activex control see pages 105 109 m Soft keys and menu driven functions with on line help power meter in low light conditions Selected Screens Digital Power Screen CW industrial medical and scientific lasers pW to Multi kW with appropriate sensors Fast response bar graph BeamTrack Power Position Size Screen Monitoring of laser beam size m Accurate tracking of beam position to fractions of a mm
101. s caer sow FBS cow ee coe oe Obey Ophir Opens Arab Here multi line histogram display has been chosen BeamtTrack Power Position Size sensor Power Le Position Size Here a BeamTrack position and size graph is shown Q OPHIR 01 08 2013 __ Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand 2 3 2 Starcom This software is supplied with the Nova Il Laserstar Vega and Nova with RS232 option It allows you to measure analyze and record power and energy from any Ophir sensor You can log the data from each sensor simultaneously to file rrr Plot of ratio of energy B A vs energy A Plot of power vs time Histogram plot of energy distribution System Integrator Solutions Besides their use as stand alone fully featured laser power energy meters Ophir devices are easily incorporated into larger end user applications This allows system integrators to leverage Ophir s excellence in measurement capabilities with legacy analysis packages 2 3 2 BONNclmNAleinelas Communication Protocols All Ophir devices support one or two forms of communication with the PC Device RS232 USB GPIB Bluetooth Pulsar Vega e Nova ll USB Interface Nova LaserStar e Quasar Juno RS232 RS232 communication is the simplest to integrate into your OEM application Integrated Development Environme
102. sensors PD300 BB Flat spectral response from 430 to 1000nm 10x10mm 430 1000nm 50pW 4mW 26 PD300 BB 50mW For broadband light sources to 50mW 10x10mm 430 1100nm 50pW 50mW 26 PD300 CIE Measurement in units of Lux or foot candles 2 4x2 8mmM 400 700nm 20mLux 200kLux 26 BC20 Meter for scanned beams at up to 30 000 inch s 10x10mm 633 650 675nm 100uUW 20mW 26 Special sensors integrating spheres 3A IS Integrating sphere for divergent beams to 3W O12mm 420 1100nm 1 uW 3W 2 3A IS IRG Integrating sphere for divergent beams to 3W for near IR 12mm 800 1700nm 1 uW 3W 27 Thermal Power Sensors High sensitivity thermal sensors 30uW 12W Sensor Features Aperture Spectral Range Power Range Energy Range Page 3A Very low powers 9 5MM 0 19 20um 60uW 3W 20uJ 2J 28 3A P Low powers and energies O12mm 0 15 8um 60UW 3W 20uJ 2J 28 3A P THz 3A P sensor calibrated for Terahertz wavelengths O12mm 0 3 10THz 50uW 3W 20uJ 2J 28 3A FS Lowest powers Fused Silica window 9 5MM 0 19 20um 30uW 3W 15uJ 2J 28 3A P FS 12 For divergent beams window blocks infrared O12mm 0 22 2 1um 60uUW 3W 20uJ 2J 28 12A Wide dynamic range to 12W O16mm 0 19 20um 2mW 12W 1mJ 30J 29 12A P Short pulse lasers to 12W O16mm 0 15 8um 2mW 12W 1mJ 30J 29 Low power thermal sensors 20mW 50W Sensor Features Aperture Spectral Range Power Range Energy Range Page 10A General purpose to 10W O16mm 0 19 20uUM 20MW 10W 6mJ 25 30 30A BB 18 General purpose to 30W O17 5mm 0 19 20um 20mW 30W 6mJ 30J 30 L30A 10MM T
103. size e 3rd 2 Quad 1 2 BSfelarsrelas qst Quad Beam size detector 4 Quad Total output Operation of BeamTrack Sensors BeamTrack sensors look similar to Ophir thermal sensors of the same type except that there is a small electronics module on the cable from the sensor head to the smart plug When BeamTrack sensors are plugged into compatible displays or PC interfaces Nova II Vega StarLite and Juno along with the power measurement there is a visual display of the beam position and beam size The beam position can be accurately tracked and logged for beam wander measurements The beam size is calibrated only for Gaussian beams but other beams may be measured and the sensor will give a repeatable measurement of the relative beam size for tracking changes in the size of the beam over time Q OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand 1 2 3 Qxelawelas 01 a 2 o HIR 1 2 1 BeamTrack Power Position Size Sensors 100uW to 10W Features All the features of standard power sensors plus Accurate tracking of beam position to fractions of amm Monitoring of the laser beam size 3A QUAD 3A P QUAD 10A PPS Model 3A QUAD 3A P QUAD 10A PPS Use General purpose Short pulses Low power Functions Power Energy Position Power Energy Po
104. software OPHIR 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 2 2 PC Interfaces 2 2 1 Compact Juno USB Interface Convert your laptop or desktop PC into an Ophir sensor power energy meter From sensor to interface to PC no power source needed Plug and play with all standard Ophir smart sensors Position amp size measurement with BeamTrack sensors Record every energy pulse at up to 10kHz Log power and energy average statistics histograms and more with included StarLab application LabVIEW VIs and COM Object interface m Very compact is just an extension of the smart plug Ca Smart Sensor to Juno to PC D 4H Ophir s basic smart compact Juno module turns your PC or laptop into a full fledged Ophir laser power energy meter WU Just install the software plug the sensor into the Juno module and connect the Juno with a standard USB cable to the PC USB port Using the Juno you can connect several sensors to the PC by using one Juno module for each sensor and if necessary a USB hub D c O ik Lis X wll di AA NA N H oE LabVIEW Juno operating with StarLab software Juno with BeamTrack sensor and StarLab showing beam power position and size Specifications Power Measurement Power log period 5s to 500hr Energy Measurement Max real time datalogging to PC 10 000 Hz Trigge
105. source System incorporates 16 bit digitizer light scatter control and special amplifiers to achieve higher dynamic range than standard LD8900 For pulsed operation please consult the factory Item Description P N LD8900 InGaAs Goniometric Radiometer for characterizing the angular radiation intensity from a laser diode between PH00173 800nm and 1700nm wavelength Entrance aperture 2mm LD8900 Si Goniometric Radiometer for characterizing the angular radiation intensity from a laser diode between PH00174 320nm and 1100nm wavelength Entrance aperture 2mm Full 3D capability Features dynamic range gt 36dB with O dB source LD8900R InGaAs Wide Dynamic Range Goniometric Radiometer for characterizing the angular radiation irradiance from PH00175 a fiber optic wave guide laser diode VCSEL or LED between 800nm and 1700nm wavelength LD8900F Si Wide Dynamic Range Goniometric Radiometer for characterizing the angular radiation irradiance from PH00176 a fiber optic waveguide laser diode VCSEL or LED between 320nm and 1100nm wavelength Full 3D capability Options SS WL O Wavelength option PH00183 Pulsed Failsafe operation for pulsed sources operating at repetition rates gt 10kHz with pulse widths gt 500ns PH00185 InGaAs Option For operation below 10kHz there are possible gain saturation states dependent on repetition rate pulse width and source power Consult the factory when operating under these conditions for
106. than 50um Accuracy for smaller beams may be worse due to the effects of insufficient resolution or pixilation In addition the effects of attenuation optics noise and proper baseline zeroing or offset compensation can have dramatic impact on the accuracy of the measurement Cameras that are not designed specifically for profiling may be much worse due to the presence of a cover glass and or IR cut off filter covering the array These optical elements must be removed for laser profiling to prevent interference fringes or distortion of the beam being tested Camera arrays provide a true two dimensional picture of the beam and will show fine structure and hot and cold spots which a slit will integrate out Some applications do not require a map of the laser power distribution with in the spot Spot size and spot location are sufficient Other applications require that a careful mapping of the complete mode structure is made These applications require 2D array based sensors The accuracy requirement is a question of what the data is to be used for Accurate collimation or focus control requires the highest beam size accuracy Checking the laser for hot spots uniformity or beam shape dictates that the 2D sensor is employed and is as important as absolute size measurement accuracy How and where a profiler is to be used is also an important consideration in the equation Profilers used by research and development scientists are often specialized Ease of use a
107. the junctions are in series and the hot junctions are always on the inner hotter here side and the cold junctions are on the outer cooler side radial heat flow on the disc causes a voltage proportional to the power input Laser power impinges on the center of the thermopile sensor disc on the reverse side of the thermopile flows radically and is Hot cooled on the periphery The array of thermocouples measures the temperature gradient nen which is proportional to the incident or absorbed power In principle the reading is not Cold dependent on the ambient temperature since only the temperature difference affects the junction voltage generated and the voltage difference depends only on the heat flow not on the ambient temperature Since all the heat absorbed flows through the thermocouples as long Suit as the laser beam is inside the inner circle of hot junctions the response of the detector is almost independent of beam size and position If the beam is close to the edge of the inner circle some thermocouples become hotter than others but since the sum of all of them is measured the reading remains the same Generally Ophir specifies 2 uniformity of BeamTrack Power Position Size sensors Ophir now has the new BeamTrack thermal sensor that can measure beam position ond 3st and beam size as well as power This innovative device provides an additional wealth of Quad information on your laser beam centering beam position and wande
108. to 10W 16mm 0 19 20um 20mMW 10W 6mJ 2J 4 30A BB 18 StarLink General purpose to 30W O17 5mm 0 19 20umM 20mMW 30W 6mJ 30J 42 50 150 A BB Power position amp size to 50W 150W intermittent O26mm 0 19 20UmM 40mW 150W 20mJ 100J 42 26 PPS StarLink 30 1 De CW to 30W intermittent to 150W O17 5mm 0 19 20um 30mMW 150W 20mJ 100J 42 18 StarLin L50 150 A StarLink CW to 50W intermittent to 150W large aperture O50mm 0 19 20uUm 100mW 150W 100mJ 300J 42 ine aaa Power position amp size to 250W large aperture O50mm 0 19 20uUm 150mMW 250W 80mJ 300J 4 StarLin 1000W StarLink Water cooled to 1000W O34mm 0 19 20uUm 5W 1000W 300mJ 300J 42 1 0 RENKON 9 Q OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics 01 08 2013 Power Sensor Accessories Accessories for PD300 sensors Fiberoptic adapters Accessory Description Page PD300 F O adapters Adapters for mounting fibers to PD300 sensors ST FC SMA SC 43 Accessories Accessory Description Page co PD300 CDRH 7mm aperture adapter for CDRH measurements 43 N C Accessories for thermal sensors U Fiberoptic adapters a Accessory Description Page O Thermal F O adapters Adapters for mounting fibers to thermal sensors ST FC SMA SC 44 _ Accessories for PD300R PD300 IRG 3A IS and FPS 1 Fiberoptic adapters Accessory Description Page F O Adapters Adapters for mounting fibers to PD3
109. website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand OPHIR Photonics A Newport Corporation Brand OPHIR Photonics A Newport Corporation Brand 215 01 08 2013 216 01 08 2013 Product P N Page Lens 400 2um PHOO224 194 lens 400mm LIR PH00242 194 Lens 400mm NIR PHOO240 194 Lens 400mm VIS PH00238 194 LENS 400 UV XXX PH00091 194 LPK CO 6 4 0 5 SP90075 202 LPK CO gt 6 4 5 0 SP90076 202 LPK CO gt 16 0 5 SP90077 202 LPK CO 16 5 0 SP90078 202 LPK YAG 2 5 USB SP90168 201 LPK YAG 7 USB SP90169 201 LPK YAG 16 USB SP90170 201 M 200s FW SP90144 189 M 200s FW A SP90145 189 M 200sM FW SP90146 189 M 200sM FW A SP90147 189 Mfgsoft PH00210 210 MODECHECK CO2 5kW SP90211 204 ModeCheck storage carrying case SP90227 204 Model 1740 PH00074 194 Model USB NFP 980 NS PH00230 185 Model USB NFP 1550 NS PH00229 185 Model USB NFP Pyro PH00232 185 Model USB NFP VIS NS PH00231 185 Mounting Hardware 5000W detector SP90212 204 Mounting Hardware 10 000W detector SP90213 204 MS 1780 PHO0096 191 MS NIR Kit PHOO111 191 MS NIR Lens Kit PHOO111 191 MS TUBE Kit PHOO127 191 MS UV Kit PHOO097 191 MS VIS Kit PHOO104 191 MS VIS Lens Kit PHOO104 191 MS YAG Kit PH00118 191 MSP NS Pyro 20 25 PH00218 194 ND1 nom x10 attenuator 7 Z08200 78 ND1 stackable filter red housing SPZ08234 172 ND2 nom x50 attenuato
110. www ophiropt com photonics A Newport Corporation Brand Sensors Q OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand Sensors Table of Contents Power sensors Photodiode Power Sensors Standard photodiode sensors 10pW 3W A Sensor Features Aperture Spectral Range Power Range Page PD300 Automatic background subtraction 10x10mm 350 1100nm 500pW 300mW 22 N PD300 1W Automatic background subtraction 10x10mm 350 1100nm 500pW 1W 22 Cc PD300 3W High power 10x10mm 350 1100nm 5nW 3W 22 aD PD300 TP Very thin profile 4mm only 10x10mm 350 1100nm 50pW 1W 22 LS PD300 UV Wide spectral range and low noise 10x10mm 200 1100nm 20pW 300mW 23 PD300 IR Infrared O5mm 700 1800nm 5nW 300mW 23 O PD300 IRG Very low noise 300 femto watts 5mm max 800 1700nm 10pW 150mW 23 D Round photodiode sensors 20pW 3W Sensor Features Aperture Spectral Range Power Range Page PD300R Same as PD300 circular for easy centering 10mm 350 1100nm 500pW 300mW 25 PD300R 3W Same as PD300 3W circular geometry 10mm 350 1100nm 5nW 3W 25 PD300R UV Same as PD300 UV circular geometry 10mm 200 1100nm 20pW 300mW 25 PD300R IR Same as PD300 IR circular geometry O5mm 700 1800nm 5nW 300mW 25 Special photodiode sensors and integrating spheres 50pW 3W and 20mLux 200kLux Sensor Features Aperture Spectral Range Power Range Page Special photodiode
111. 0 of For wavelengths below 240nm derate to 1J cm above value For beam size lt 5mm For 10mm beam derate to 50 of above values Notes c With the user threshold setting set to minimum For other settings the spec is for gt 7 of full scale or greater than twice the user threshold whichever is greater The user threshold is available with Nova Il Vega StarLite or Juno For other meters the threshold is set to minimum and the linearity spec is gt 10 of full scale The PE C series will only operate with Nova or Orion meters with an additional adapter Ophir P N 7Z08272 see page 77 The adapter can introduce up to 1 additional measurement error The user threshold feature allows adjustment of the internal threshold up to 25 of full scale if desired to avoid false triggering in noisy environments The user threshold setting represents the approximate minimum energy for pulse widths below 50 of the pulse width setting For longer pulse widths the actual minimum may be higher For highest accuracy it is recommended to zero the sensor against the meter the first time it is used with a particular meter For further information see the FAQs on our Website Notes d A shock absorbing mounting post is available for situations in which sensor is mounted on a surface subject to shock or vibration This can prevent false triggering and allow working at lower minimum energies Note however that in this case the maximum average power will be reduced
112. 0 1 10ms short pulses lt 1us and continuous radiation Absorbers optimized for long pulses and CW are characterized by thin refractory materials since the heat can flow through the coating and into the disc during the pulse On the other hand heat cannot flow during short pulses and all the energy is deposited in a thin typically 0 1um layer near the surface This causes vaporization of the surface which ruins the absorber Instead a volume absorber that is partially transparent and absorbs over a distance of 50um 3mm is used This spreads the heat over a larger volume allowing much higher energies Ophir thermopiles can measure from tens of microwatts to Kilowatts Nevertheless the thermal range of operation of the discs is limited If the difference between the hot and cold junction temperature exceeds tens of degrees the constant heating cooling of the junctions can cause premature failure in the junctions In order to accommodate different power ranges discs of different thicknesses and sizes are used thick ones for high powers and thin ones for low powers The response time of the discs is dependent on their size and shape larger diameters and thicker discs are slower than thin small diameter ones The response time is in general dependent on the mass of material which has to heat up in the thin absorber region of the disc vs 2 OQ OPHIR 01 08 2013 __ Photonics For latest updates please visit our website www ophiropt com phot
113. 0 NIR Beam splitter and attenuators beam split 2 times SP90185 FSA 50Y Negative lens 50 mm YAG SP90187 N FSA 100Y Negative lens 100 mm YAG SP90188 YY FSA 125Y Negative lens 125 mm YAG SP90189 FSA 150Y Negative lens 150 mm YAG SP90190 FSA 200Y Negative lens 200 mm YAG SP90191 Accessories WVF 300 ND filters variable wedge Replaces fixed value filter slides SP90195 BD 040 A Beam Dump 40 Watts max power air cooled SP90192 BD 500 W Beam Dump 500 Watts max power water cooled SP90193 156 Y OPHIR Y Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Ga Corporation Brand A Newport Corporation Brand Newport Corporation Brand 3 3 Introduction to Scanning Slit Profilers The scanning slit beam profiler moves two narrow orthogonal slits in front of a linear photo detector through the beam under analysis Light passing through the slit induces a current in the detector Thus as the slit scans through the beam the detector signal is linearly proportional to the spatial beam irradiance profile integrated along the slit A digital encoder provides accurate slit position The photo induced current signal is digitized and analyzed to obtain the beam profile in both X and Y from the two orthogonal slits The slit apertures act as physical attenuators preventing detector saturation for most beam applications High dynamic r
114. 00R PD300 IRG 3A IS and FPS 1 spectrum analyzer ST FC SMA SC 44 General Accessories Accessories Accessory Description Page SH to BNC Adapter Allows connection of sensor to voltage measuring device for measurement of raw voltage output 44 IR Phosphor Card Glass slide 75x25mm with phosphor coating 25x50mm that visualizes spectral region 810 860nm 900 1100nm and 44 1500 1600nm Stands up to 1kW cm and 0 5J cm Self actuating does not need charging from light source High power water cooled and fan cooled laser beam dumps Accessories Accessory Description Page BDFLS00A BB 50 Fan cooled to 500W general purpose high power beam dump 45 BD5000W BB 50 Water cooled to 5000W general purpose high power beam dump 45 BD10K W Water cooled to 10000W general purpose high power beam dump 45 OEM Thermal Sensors Standard OEM thermal sensors 20mW 250W Sensor Features Aperture Spectral Range Power Range Size Page 20C SH Compact smart sensor O12mm 0 19 20um 20mMW 20W 38x38x14mm 49 20C A Compact built in amplifier analog O12mm 0 19 20UmM 200mMW 20W 38x38x34mm 49 20C UAU Compact external amplifier USB connection O12mm 0 19 20uUm 20mW 20W 38x38xl4mm 49 L30C SH Medium aperture smart sensor O26mmM 0 19 20um 80mW 50W 60x60x38mm 50 L30C UA Medium aperture built in amplifier RS232 connection 26mm 0 19 20um 80mMW 50W 60x60x38mm 50 L30C UAU Medium aperture built in amplifier USB connection 26mm 0 19 20umM 80mW 50W 60x60x38mm 50 100C SH Low profil
115. 00W 2J to Z00 2J to 200uJ 2J to 200uJ 2J to 200 Minimum Energy 20uJ 20uJ 20uJ 15uJ 20 Maximum Energy Density J cm lt 100ns 03 1 0 1 03 1 0 5ms 1 1 1 1 1 2Ms 2 2 10ms 4 4 Cooling convection convection convection convection convection Weight kg 0 2 02 02 0 2 OS Fiber Adapters Available see page 44 ST FC SMA SC ST FC SMA SC ST FC SMA SC ST FC SMA SC NA Version V1 Part number Standard Sensor 7Z02621 7Z02622 7Z02742 7Z02628 7Z02687 BeamTrack Sensor Beam Posivtion amp Size p 56 7Z07934 7Z07935 StarLink Sensor Direct USB link to PC p 42 787000 787001 787002 Note a Note b Note c Note d Note e For P type and shorter wavelengths derate maximum energy density as follows Depending on room airflow and temperature variations Remove window for measurement beyond 2 2um 2 sigma standard lab traceable for gt 0 6THz For 0 5THz and below add 5 to error Back reflections from meter can sometimes cause interference effects with source Unit should be tilted 10 in this case Wavelength 1064nm 532nm 355nm 266nmM 193nm Derate to value Not derated Not derated 40 of stated value 10 of stated value 10 of stated value REMOVABLE PART pf 18 97 14 ADJUSTABLE 1 75 01 08 2013 2 OPHIR SS Photonics A Newport Corporation Brand Newport Corporation Brand 3A P 3A P THz REMOVABLE PART
116. 0108 a PY III W Poly THZz Pyrocam Ill Window Polyethylene uncoated for Tera Hz wavelengths SP90208 154 Y OPHIR Y Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand Newport Corporation Brand 3 2 4 1 YAG Focal Spot Analyzer Image focal spots down to 25um in size For laser powers up to 400W additional external ND filters required Measure how focal distance shifts with power Can measure systems with focal length as short as 50mm Modular design allows flexibility in use C mount compact laser beam sampler attenuator for camera based laser beam profiling systems High damage threshold optics for measuring energetic sources Produces undistorted sample of laser under test Adjustable attenuation maximizes system dynamic range Up to 1 x 10 19 attenuation available without external filters Measure the focal spot of a relatively high power laser in particular a YAG laser The average power can be from lt 1 to 400 Watts and the focal spot can be as small as 25um The FSA can also be used to measure how the focal spot shifts with power The lasers focal length from the lens to the focal spot is usually on the order of 70 to 120mm The YAG FSA assembly adds a negative lens to the LBS 300 beam splitter assembly to increase the focal path and at the same time enlarge the image Severa
117. 0166 134 1394b FireWire Power Supply SP90167 134 1740 LENS MNT PH00075 194 1740 LENS PREP PH00076 194 1740 TRNG PH00077 194 5000W 7Z02119 40 5000W LP 7202255 40 5000W SH 7Z02119 204 Additional beam splitter SPZ17026 178 ATP K PH00128 172 Battery Pack for LaserStar 7Z14006A 94 Battery Pack for Nova 7Z11200 96 Battery Pack for Vega Nova Il Quasar 7E14007 90 92 103 BC20 7ZO2422A 26 BD10K W 7Z17202 45 BD 040 A SP90192 156 173 BD 500 W SP90193 156 173 BDS5000W BB 50 7217201 45 BDFL500A BB 50 7Z17200 45 BFC PH00205 210 Beam Cube 620 SP90323 198 Beam Dump 5kW SP90224 204 Beam Deflector Assembly SP90263 173 BeamMic to BGE Upgrade SP90230 139 BeamMic to BGP Upgrade SP90229 139 BeamMic to BGS Upgrade SP90219 139 Beam Splitter Assembly 7Z17001 76 Beam splitter for 1X UV image converter SPZ17015 181 Beam splitter for 4X UV image converter SPZ17007 181 Beam splitter for expanders SPL 17027 178 BEAMSTAR TO BGE UPGRADE SP90230 134 BEAMSTAR TO BGP UPGRADE SP90229 134 BEAMSTAR TO BGS UPGRADE SP90219 134 BGE FWB GRAS20 1550 DESK SP90253D 134 BGE FWB GRAS20 1550 LAPTP SP90253L 134 BGE FWB GRAS20 DESKTOP SP90252D 134 BGE FWB GRAS20 LAPTOP SP90252L 134 BGE GigE OSI182000 SP90269 133 BGE GigE OS1182000 1550 SP90272 133 BGE USB L11059 SP90321 ie BGE USB SP503 SP90246 133 BGE USB SP503 1550 SP90247 133 BGE USB SP620 SP90248 133 BGE USB SP620 1550 SP90249 133 k D OPHIR Spiricon Photon OPHIR Photonics A Newport Corporation Brand
118. 064nm Same Same 1 at 1064nm Same Same Same lt SP90057 LBS 100 IR 0 5 10 6um CaF2 flats 3 3mm 30 T for 3mm flat ZnSe 0 5 at Same Same Same SP90058 and 1 Imm 60 T for Imm flat 10 6um at 10 6um LBS 100 IR 5 0 10 6um Same Same ZnSe 5 at Same Same Same SP90059 10 6um LBS 100 to This adapter enables mounting of the LBS 100 beam splitter attenuator assembly in front of the 4X beam reducer SPZ17029 4X beam The combined assembly can image large high power beams in one unit reducer adapter VO OPHIR Spiricon Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand 3 4 3 Beam Splitter Single amp Dual Front Surface Model Beam Tap amp Il Beam Tap amp II YAG Stackable Beam Splitter Beam Samplers Wavelength 400 700nm 1064nm 190 2000nm 200nm 2 5um Reflection 4 amp 0 16 of incident beam 0 5 amp 0 0025 of incident beam 5 amp 0 025 of incident beam 0 057 532nm Clear aperature O17 5mm O17 5mm 15mm O14mm Damage threshold 5W cm no distortion 5W cm no distortion gt 5 J cm 100MW cm Mounting C Mount Threads C Mount Threads C Mount Threads C Mount Threads Beam Tap amp Il m Dual surface reflector for equalizing S amp P polarization m The two planes of reflection are orthogonal Single Surface Polarization Problems A single surface reflection at 45 is often used to sample a
119. 0mJ Lowest Measurable Energy 0 01 0 01 0 06 0 08 0 1 OCs 0s 0E 04 05 04 07 Ls Iss 15 2 3 5 5 5 mJ ed Max Pulse Width ms 0002 00m 05 1 5 000A OVEM 05 1 5 1 2 5 10 20 1 2 5 10 20 Maximum Pulse Rate pps 10kHz 5kHz 800Hz 400Hz 100Hz 10kHz 5kHz 800Hz 400Hz 100Hz 200 100 50 35 25 200R CO se 35 25 Noise on Lowest Range uJ 1 1 6 10 20 5 5 30 50 100 80 10 1250 o0 20 SUC SOC CCCs SUC 1600 Additional Error with O eso fae E T o E e Pen E 1 Frequency 2kHz to 2kHz to 4 5 80Hz 45 80Hz to KHz to SkHz Linearity with Energy for gt 1 5 1 10 of full scale Damage Threshold J cm2 lt 100ns 0 1 1 5 0 8 3 lus 0 2 3 3 300us 2 20 5 10 2ms 6 60 10 25 Maximum Average PowerW 15 25 with optional heat sink 40 60 with optional heat sink 15 40 Maximum Average Power 20 500 20 500 Density W cm Weight kg 0 3 1 2 Version Part Number 7Z02948 7Z02942 Previous Model Part Number 7Z02867 7Z02890 Notes a Calibrated at 532nm and 1064nm Calibrated at 1064nm Calibrated at 532nm Calibrated at 532nm 1064nm and only 2100nm and 2940nm and 1064nm only 1550nm only Notes b With the user threshold setting set to minimum For other settings the spec is for gt 10 of full scale or greater than twice the user threshold whichever is greater The user threshold is available with Nova Il Vega StarLite or Juno For other meters the threshold is set to minimum and the linearity spec is gt 10 of full scale The PE C series will only operate with Nova or Orion met
120. 0nm to 1100nm TI Antireflection Coating Antireflection coating optimized for 1064nm and 532nm Beam reduction Accuracy 390 mM Size 60 mm dia x 94mm length Aperture 50mm Maximum Beam Size SP 503 FX50 25x19mm FX 33 18x14mm SP 620 or GRAS20 28x21 2mm Distortion of Beam Less than 1 over 80 of diameter Damage Threshold 30mJ per pulse for nanosecond pulses Ordering Information 4X Imaging Beam Reducer Item Description P N 4X reimaging beam reducer Screw on beam reducer for beams in the wavelength region 360 1100nm that reimages the beam 30cm infront of SPZ17017 the unit onto the CCD while reducing the beam size 4X Entrance aperture is 50mm Fits 4 5mm recess cameras only Accessories Filter holder and 50x50 filter set Filter holder with set of 4 standard Schott 50X50mm neutral density filters Useful to further reduce intensity after SPZ08240 for 4X beam reducer beam splitter before inputting into 4X beam reducer Mounts to standard 1 4 thread 2 diameter laboratory rod LBS 100 to 4X beam reducer This adapter enables mounting of the LBS 100 beam splitter attenuator assembly in front of the 4X beam SPZ17029 adapter reducer The combined assembly can image large high power beams in one unit See illustration on page163 Y OPHIR Spiricon Photonics For latest updates please visit our website www ophiropt com photonics Soy eee ES 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport
121. 1 154 PY III W Ge 10 6 SP90105 154 PY III W Ge 3 5 5 SP90104 154 PY III W Ge 8 12 SP90106 154 PY III W Poly THz SP90208 154 PY III W Si 1 05 2 5 SP90102 154 PY II W Si 2 5 4 SP90103 154 PY III W ZnSe 10 6 SP90107 154 PY II W ZnSe 2 5 SP90108 154 Quasar 7201300 87 103 RAL FXT PH00073 167 REF PH00204 210 RS232 Cable for LaserStar 7E01121 94 RS232 Cable for Vega and Nova II 7E01206 90 92 RSP100 PH00078 167 RSP200 PH00079 167 RSP500 PHO0080 167 SC fiber adapter 7208227 44 76 78 Scope Adapter 1Z11012 76 SH to BNC Adapter 7Z11010 44 Shock Absorbing Mounting Post 7Z08268 77 SMA fiber adapter 1G01236 44 76 78 Spacer assy for objectives SPZ08261 178 ST fiber adapter 7Z08226 44 76 78 StarLite 7Z01565 86 98 USB A B Cable SP90204 134 USB A mini B Cable SP90205 134 USB Cable for Juno 701217 101 USB Cable for Vega and Nova ll 7E01205 90 92 USB Interface legacy 7Z01200 102 USB MSP HPNS 10 5 PHO0236 194 USB MSP NS Ge 9 5 PH00234 194 USB MSP NS Pyro 9 5 PH00235 194 USB MSP NS Si 9 5 PH00233 194 USB NS Ge 3 5 1 8 PRO PHOO020 165 USB NS Ge 3 5 1 8 STD PHO0391 165 lt Q OPHIR Spiricon Photon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics OPHIR Photonics A Newport Corporation Brand a Corporation Brand A Newport Corporation Brand A Newport Corporation Brand Product P N Page USB NS Ge 9 5 PRO
122. 1 PERMENO Input from laser Host Laser System bending mirror and focusing lens Beam Cube Beam Cube Input lens Adjustment rods CCD Beam splitter assembly simplified beam profiler Optical trigger for automatic synch with pulsed lasers and temporal profile RP power energy temporal profile head Q OPHIR Spiricon Photonics For latest updates please visit our website www ophiropt com photonics A 01 08 2013 A Newport Corporation Brand A Newport Corporatio 3 7 1 ERMENE 198 Specifications General Max and min average power Maximum average power density Max and min energy Maximum energy density pulse width and repetition rate at Beam Cube 1W to 100W continuous and to 150W for up to 1 min AkW cm2 at entrance window entrance window vs pulse 2ms width Cooling System Dimensions Spectral Range Beam profiler unit Camera PC interface Shutter speeds Gain control Frame rate at 640x480 pixel ROI Software features Minimum PC system requirements Intensity adjustment System optical performance Field of view Maximum beam size Beam reduction or expansion Resolution Power energy temporal profile unit Temporal pulse shape response time into oscilloscope Software functions with USB Interface connected to PC or laptop Data logging 20mJ to 100Joules max energy density i 10ms 20J cm ms ooo 5J cm f 0 5ms 1 5J5 cm 2 Conduction cooled 22cm Lx 16cm W
123. 1000W high power densities and long pulses 34mm 0 4 1 5um 10 6um 5W 1000W 300m4J 300J 39 L1500W Water cooled to 1500W O50mm 0 19 20umM 15W 1500W 500m4J 200J 39 L1500W LP As above high power densities and long pulses O50mm 0 4 1 5um 10 6um 15W 1500W 500mJ 2005 39 5000W Water cooled to 5000W O50mm 0 19 20umM 20W 5000W N A 40 5000W LP As above high power densities and long pulses 50MM 0 4 1 5um 10 6um 20W 5000W N A 40 10K W Water cooled to 10 000W highest power densities O45mm 0 8 2um 10 6um 100W 10 000W N A 40 Comet 1K Portable low cost power probe for low powers 50MM 0 2 20um 20W 1000W N A 41 Comet 10K Portable low cost power probe for high powers 100mm 1 06um and 10 6um 200W 10 000W N A 41 Comet 10K HD Portable low cost power probe with high damage 55MM 1 06um and 10 6um 200W 10 000W N A 41 threshold StarLink Direct to PC Power Sensors Sensor Features Aperture Spectral Range Power Range Energy Range Page PD300 StarLink Photodiode general purpose to 300mW 10x10mm 350 1100nm 500pW 300mW N A 42 3A StarLink Very low powers to 3W 9 5MM 0 19 20uUmM 60UW 3W 20uJ 2J 42 3A QUAD StarLink Power amp position very low powers to 3W 9 5mm 0 19 20um 100uW 3W 20uJ 2J 42 3A P StarLink Low powers and energies O12mm 0 15 8um 60UW 3W 20uJ 25 42 3A FS StarLink Lowest powers to 3W Fused Silica window O9 5mm 0 19 20um 30uW 3W 15uJ 2J 42 10A StarLink General purpose to 10W O16mm 0 19 20um 20mW 10W 6mJ 2J 42 10A PPS StarLink Power position amp size
124. 102 6671 802 juergen reingruber eu ophiropt com o Argentina Sirex Medica S A 54 11 4816 4585 andresc sirex com BeNeLux Ophir Spiricon Europe 49 4102 6671 802 reingruberj spiricon de e Brazil ee 55 11 2910 6852 ettore photonics com br s 3 Brazil Lynx Com Imp Ltda 55 11 3862 2099 vendas lynxbrasil com br Bulgaria ASTEL 359 29 587 885 86 89 n georgiev astelbg com China Ti Electro Optics Co 86 10 6263 4840 lake lu teo com cn Colombia Reyes Puyana Ltda 57 7 643 53 07 reyespuyana gmail com e e Cyprus Vosimcon Medical Ltd 357 2463 3621 vosimcon cytanet com cy e s Czech Republic MIT s r o 420 241 712 548 info mit laser cz 8 e e Denmark Ophir Photonics 972 2 5487414 Yoram Shalev ophiropt com e e Finland Cheos Oy 358 201 98 64 64 kim grundstrom cheos fi France Ophir Spiricon Europe 49 4102 6671 802 reingruberj spiricon de Georgia Intermet Ltd 995 32 518 303 david intermet ge e e Germany Ophir Spiricon Europe 49 41 02 6671 802 reingruberj spiricon de e Greece Acta Ltd 30 210 600 3302 ageo acta com gr e Hong Kong Titan Electro Optics 86 755 8320 5020 jimmy xiao teo com cn e 6 Hungary Quantum Lasertech 36 30 539 1501 ugrai gabor quantumlasertech hu e India New Age 91 124 408 6513 support newagein com e Indonesia Inno V Global 65 6296 1217 daphne innov global com o e Ireland Ophir Spiricon Europe 49 4102 6671 802 juergen reingruber eu ophiropt com o e e Isra
125. 12V charger input Ordering Information Item Description Ophir P N Quasar Bluetooth Module to operate one Ophir sensor from your PC via Bluetooth wireless interface Comes with software Max 7Z01300 Interface repetition rate for every pulse 500Hz Powered from built in rechargeable battery Comes with power supply Bluetooth adapter required when not available on PC See next line USB to Bluetooth Adapter for PC or Laptop not equipped with built in Bluetooth This adapter is tested and recommended by Ophir 7E10039 adapter Quasar is not guaranteed to work with all other adapters on the market Battery Pack for Quasar Replacement battery pack for Quasar 7E14007 103 Q OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand Summary of Computer Options for Ophir Meters and Interfaces Communications With Ophir RS232 USB Bluetooth and GPIB communication options you can transfer data from the sensor to the PC in real time or offline You can also control your Ophir power meter from the PC USB standard on Nova Il Vega power meters and Juno Pulsar and USBI PC interfaces Bluetooth wireless on the Quasar interface RS232 standard with the Laserstar Nova Il and Vega optional on the Nova GPIB optional with the Laserstar Ophir Power Meter and Interface Specifications Model Nova Laserstar Nova II Vega StarLite Puls
126. 150C UAU Consult Ophir representative 53 L250W 7Z02688 38 L250W UA Consult Ophir representative 53 L250W UAU Consult Ophir representative 53 L300W LP 7Z02689 38 L300W UA Consult Ophir representative 53 L300W UAU Consult Ophir representative 53 L1500W 7202661 39 L1500W LP 7Z02665 39 L1500W LP1 RP 7202919 73 Large aperture 1st Wedge Beam Splitter SPZ17025 177 Large C mount Wedge Splitter SP90273 FE LaserStar Dual Channel 7Z01601 86 94 LaserStar IEEE Option 78300 94 99 LaserStar Single Channle 7Z01600 86 94 LBA TO BGE UPGRADE SP90232 134 LBA TO BGP UPGRADE SP90231 134 LBA TO BGS UPGRADE SP90210 134 LBF 50 filter set SP90081 172 LBS 100 SP90061 174 LBS 100 IR 0 5 SP90058 174 LBS 100 IR 5 0 SP90059 174 LBS 100 to 4X beam reducer adapter SPZ17029 174 179 LBS 100 YAG SP9005 7 174 LBS 300 BB SP90186 139 173 LBS 300 NIR SP90185 156 173 LBS 300 UV SP90183 173 LBS 300 VIS SP90184 173 LD8900 HD PH00198 210 LD8900 InGaAs PH00173 208 LD8900 Si PH00174 208 LD8900R InGaAs PHOO175 208 LD8900R Si PH00176 208 LD8900 Software Viewer PH00181 208 LD8900R Software Viewer PH00439 208 LED Profiler PH00199 210 LED profiler w 3180 PH00200 210 Legacy Software PH00420 166 LENS 100 LIR PH00095 194 LENS 100 NIR PH00094 194 LENS 100 VIS PH00093 194 LENS 190 10 6 PH00092 194 Lens 200mm LIR PH00241 194 Lens 200mm NIR PH00239 194 Lens 200mm VIS PH00237 194 LENS 200 UV XXX PH00090 194 Q OPHIR Spiricon Photon Photonics For latest updates please visit our
127. 17 14 5 95 140 75 7 i 100 1 l 75 l b For 10 50 z derate as follows Wavelength Derate to value 1064nm Not derated 532n Not derated 355n 70 of stated value 266nmM 15 of stated value 193nm 10 of stated value Q Damage threshold 1 5J cm for wavelengths lt 500nm HIR Y Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand 1 1 2 3 Low Medium Power Thermal Sensors Apertures to 35mm 50mW to 150W Features Special purpose SV and HE absorbers 30 150 A SV 17 30 150 A HE 17 Diffuser installed 30 150 A HE DIF 17 Diffuser off For concentrated beams and pulses l N Convection air cooled vs CW to 30W intermittent to 150W 17mm aperture U N i Model 30 150 A SV 17 30 150 A HE 17 30 150 A HE DIF 17 N Use High power and energy density High energy and average power Concentrated beam pulsed m pulsed lasers lasers has removable diffuser Absorber Type SV HE HE Spectral Range um 0 19 12 0 19 0 625 1 064 2 1 2 94 0 19 3 except for 0 625 0 9 Aperture mm o1 7mm o1 7mm o1 7mm Power Mode Power Range 100mW 150W 50mW 150W 50mW 150W Maximum Intermittent Power W 150W for 1 5min 100W for 2 2mi
128. 24203 E p631392 00 A2003 T568019e 03 ui Centroid IO 21 Te 09 2637 oie 220960 1LeL SoS Fle OF 25065 5e 03 um Peak Loc X 50 19755 0 1ii2e 03 fOr 6a5e 05 h6112e 05 dimet wm Peak Loe Y 1510 LPM Jiapiie ji L3sb0le 03 5 27 5600 03 ioe OL a D4ex 1650 BOPSe 04 BOSS O EE aE T Ea i ELOR 03 als P E um Digt BO ilie GO Sei E ai i ble 03 5 998e 3 um Dio EO 7i le 03 Tie 03 LiSe 1 Tatile Titde 03 um Failures or successes can be the impetus for additional actions including a TTL output signal or PC beep and the termination of further data acquisition Q OPHIR Photonics A Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics 3 2 1 1 PERMES 23 Spiricon OPHIR Photonics A Newport Corporation Brand 01 08 2013 Camera Compatibility For lasers between 190 1320nm wavelenghts BeamGage interfaces to silicon CCD Firewire 1394 and USB cameras For applications between 1440 1605nm BeamGage supports cost effective phosphor coated CCD cameras For demanding applications between 900 1700nm BeamGage supports an InGaAs camera And for applications in the ultraviolet 13 355nm or far infrared or Terahertz range 1 06 3000nm BeamGage supports Spiricon s Pyrocam Ill pyroelectric array camera 190 1100nm Model SP503U SP620U GRAS20 Gevicam L11059 Spectral Response nm 190 1100nm 190 1100nm 190 1100nm 190 1100nm 190 1100nm Application Y2
129. 3 Laserstar Versatile Laser Power Energy Meter Two models available dual and single channel m Single channel model can be upgraded to dual channel Compatible with all Ophir thermopile pyroelectric photodiode and RP sensors Large LCD display Backlighting and rechargeable battery Screen graphics and statistics std dev min max Analog output Built in RS232 interface Log every data point at gt 1500Hz with pyroelectric sensors Non volatile data storage up to 54 000 points Laser tuning screen and power log Audio sound for laser tuning and low battery RS232 interface with Starcom PC application software and LabVIEW driver see pages 107 109 GPIB option IEEE488 1 IEEE 488 GPIB Cable for NIST traceable LaserStar CE marked Soft keys menu driven The dual channel model enables user to simply plug in any of Ophir s thermal pyroelectric photodiode or RP sensors and measure two channels independently or the ratio or difference between them in real time Up to 10 data files 54 000 points total can be stored for onboard review or downloading to computer even if Laserstar has been switched off The built in RS232 interface and Starcom PC software allow on line processing of data or processing previously stored data results are displayed graphically on a PC To support PC interfacing LabVIEW drivers are provided 1 3 BOWielaWleiteles 153 00uJ F aar THA LabVIEW StarCom Software Selected S
130. 30 Cooling conduction water water Output 6 pin Molex 6 pin Molex 6 pin Molex Mini B USB connector Dimensions 80x80x45mm 80x80x58mmM 80x80x58mm Part number Consult Ophir representative Consult Ophir representative Consult Ophir representative Consult Ophir representative Note a With analog UA version maximum power is also limited by maximum output voltage where output voltage is at most 2V less than input voltage Note b 4 pin Molex connections Voltage Voltage Analog signal out Ground 6 pin Molex connections RS232 input Ground Voltage Analog signal out high low voltage or switch input when used RS232 output Note c Calibrated at customer selected wavelength L150C UA L250W UA L300W UA 2x M3x10deep 62 050 a a 4x M4xBdeep N i E P S 70 MOLEX 6471 i S PIN 1 n a 280 122 5 45 ER 2x M3x10deep FRONT VIEW SIDE VIEW PHIR MOUNTING THREADS 2x 1 8 NPT WATER THREADS 1 1 5 1 RENLKOK 53 2 Photonics A Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics 01 08 2013 1 1 5 2 Examples of Custom OEM Power Sensor Solutions In addition to the standard OEM products described above Ophir has accumulated over 25 years experience in developing products which are tailored to precise physical configurations provided by the OEM customer These products include custom discs with or without electronics specially confi
131. 30A P 17 7202693 J 30mm diameter UV imaging plate SPF01150 181 40X SP90293 183 50 150 A BB 26 7Z02696 30 Q OPHIR Spiricon Photon Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand OPHIR Photonics A Newport A Newport Corporation Brand Brand OPHIR Photonics A Newport Corporation Brand 211 01 08 2013 212 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Terres Corporation Brand OPHIR Photonics A Newport Corporation Brand Product P N Page 50 150 A BB 26 PPS 7Z07900 od 50 150 A BB 26 PPS StarLink 787200 42 57 50A PF DIF 18 7202738 31 50mm focal length CCTV lens kit SP90038 180 50mm lens assembly SPZ08255 198 50mm X 50mm UV imaging plate SP90082 181 60X SP90292 183 100C SH 7Z02680 51 100C UA Consult Ophir representative 51 100C UAU Consult Ophir representative F 100mm X 100mm UV imaging plate SP90083 181 150C SH 77023 52 150C UA Consult Ophir representative 32 150C UAU Consult Ophir representative 52 150W UA Consult Ophir representative 52 150W UAU Consult Ophir representative 52 1000 1300nm lens 11402 001 189 1000W 7Z02664 39 1000W LP 7202668 39 1000W StarLink 787005 39 42 1394a b Adapter Cable SP90207 134 1394b FireWire Cable SP9
132. 4W free standing Minimum power 60mW 60mW 60mW Power Noise Level 3mW 3mW 3mW Maximum Average Power Density kW cm2 30 at 4W 14 at 100W 30 at 4W 14 at 100W 30 at 4W 14 at 100W Response Time 0 95 typ sec 1 2 1 2 1 2 Power Accuracy at calibration wavelength 3 3 3 Linearity with Power 1 1 1 Amplifier power supply for UA UAU versions NA 6V to 24V Via host USB Energy Mode where applicable Maximum Energy NA NA NA Minimum Energy NA NA NA Maximum Energy Density J cm lt 100ns NA NA NA 0 5ms NA NA NA 2ms NA NA NA 10ms NA NA NA Cooling conduction conduction conduction Output Ophir smart plug 6 pin Molex Mini B USB connector Dimensions 48x48x14 5mm 48x48x14 5mm 48x48x14 5mm Part number 7Z02680 Consult Ophir representative Consult Ophir representative Note a With analog UA version maximum power is also limited by maximum output voltage where output voltage is at most 2V less than input voltage Note b 4 pin Molex connections Voltage Voltage Analog signal out Ground 6 pin Molex connections RS232 input Ground Voltage Analog signal out high low voltage or switch input when used RS232 output Note c Calibrated at customer selected wavelength 100C SH 100C UA 14 5 47 6 a 19 55 14 5 A476 12 ij te 2 A i t an N H a iH Sa a leta a gepe 03 1 METER CABLE TO OPHIR 4x MSxS _ Mounting Hole SMART CONNECTOR M
133. 50A BB 35 PPS FL250A LP1 35 7Z08265 44 Fiber adapter mounting bracket for FL400A BB 50 FL250A BB 50 7208212 44 Fiber adapter mounting bracket for L40 150 A L40 150 A LP1 L50 150 A 7208238 44 Fiber adapter mounting bracket for L50 150 A BB 35 L50 150 A LP1 35 L50 150 A PF 35 7Z08265 44 Fiber adapter mounting bracket for PD300R series and FPS 1 with SM1 thread 1G02259 44 Fiber Mount BF PH00192 208 Fiber Mount FC PH00189 208 Fiber Mount SC PH00190 208 Fiber Mount ST PH00191 208 Filter for 1300nm SPZ08242 172 Filter for 355nm V2 give an undistorded image of the 355nm light SPZ08246 172 Filter holder and 50x50 filter set for 4X beam reducer SPZ08240 172 179 FL250A BB 35 7202728 36 FL250A BB 50 202759 37 FL250A BB 50 PPS 7Z07902 58 FL250A BB 50 PPS StarLink 78 201 42 58 FL250A LP1 35 7Z027315 36 FL250A LP1 DIF 33 7202733 36 FL250A RP 7202921 73 FL400A BB 50 7202734 37 FL400A LP 50 7202735 37 FL500A 7 Z02648 37 FL500A LP1 72026675S 37 FOCTUBE20 30 PH00124 191 FOCTUBE30 50 PH00125 191 FOCTUBE50 90 PH00126 191 FPS 1 fast photodiode 7Z02505 78 FSA 5OY SP90187 156 FSA 100Y SP90188 156 FSA 125Y SP90189 156 FSA 150Y SP90190 156 FSA 200Y SP90191 156 Heat Sink 7208267 76 H I 100X PH00148 167 H I 980 VIS w lens PH00146 167 H I 1550 w lens PHO0081 167 H I High energy IR PH00147 167 H I LA PHO0082 167 HP 266 PH00129 167 HP 355 PH00130 172 HP 450 PH00131 172 HP 600 PH00132 172 HP 800 PH00133 172 HP 1064 PH00134 172 HP ND1 350
134. 700 5 lt 1000 amp gt 1650 8 lt 1000 amp gt 1650 i 950 1100 7 950 1100 7 1700 1800 9 1700 1800 Damage Threshold W cm 10 50 10 50 5 50 Max Pulse Energy uJ 0 4 15 0 3 3 1 100 Noise Level for filter out pW 200 300fW at 1550 nm and 1s average Response Time with Meter s 0 2 0 2 0 2 Beam Position Dependence 2 2 1 over 80 of aperture Fiber Adapters Available see page 43 amp 44 SC ST FC SMA SC ST FC SMA FC FC APC SMA Version V1 Part Number 7Z02413 7Z02412 7Z02402 For graphs see page 24 PD300 UV PD300 IR PD300 IRG 119 5 2 118 E 5 WITH COLLIMATING LENS MOUNTING THREAD 1 4 20 BSWx6 deep i j oo d Z me a Bottom View 42 HE 5 es ADJUSTABLE 9 5 Front View Front View with filter installed with filter off Q OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand 1 1 1 1 Qfatatseyas 01 08 2013 E OPHIR Percent change per degC relative sensitivity Temperature Coefficient of Sensitivity D300 IR D300 PD300UV PD300 3W D300 IRG PD300 PD300UV PD300 3W POR00IRG POR00IRG E E CEP E Tre Vy em H Ce g 300 400 500 600 700 800 900 1000 1100 1200 1300 1400 1500 1600 1700 1800 0 9 Wavelength nm Depende
135. 706 Comet 1K Comet 10K Comet 10K HD SMART KEYS 43 145 pee ee ae lt J LASER_ABSORBER BUTTON eee SMART KEYS MAX BEAM DIAMETER 100 145 e N 4 E E y i C e E LASER ABSORBER BUTTON ON READY OFF 41 Q OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand 1 1 3 StarLink Direct to PC Power Sensors The StarLink Power Sensor Series The StarLink series is a select group of Ophir power sensors that are provided _ with the Ophir Juno USB PC interface attached The StarLink sensor is connected via a USB cable to the PC USB port and can then operate directly with the PC with no need for an Ophir power meter The StarLink package comes bundled with the celebrated Ophir StarLab software the easiest to use and most sophisticated power energy meter PC software available Alternatively StarLink sensors can be operated from the user s software via the COM Object interface provided or can work with LabVIEW via the drivers provided 1 1 3 REAALKOOL For more details about the computer interface options and
136. 7202946 65 PHO0051 167 787154 67 75 7202626 34 7Z02947 70 PHO0052 167 787155 68 75 7 Z02628 28 7Z02948 72 PH00053 167 78 156 67 75 TAUG 34 7Z07900 57 PH00070 167 787 157 69 75 702637 30 7207901 57 PH00071 167 787158 70 75 7 Z02638 29 7Z07902 58 PH00072 167 78 200 42 57 7Z026415S 35 7207904 56 PHO0073 167 787201 42 58 7202645 40 204 7207934 56 PH00074 194 787202 42 56 7 Z02648 37 707935 56 PH00075 194 787203 42 56 7Z02649 31 7Z08200 78 PHO0076 194 1G01236 44 76 78 7202651 35 7208201 78 PH00077 194 1602259 44 78 7 Z02658 35 7208210 44 PHO0078 167 1G02260 44 7202661 39 7Z08211 44 PH00079 167 1J02079 90 92 96 7202664 39 7208212 44 PHOO080 167 98 99 7Z02665 39 7208213 44 PHO0081 167 1Z11012 76 7Z02667S 37 7208216 44 PHO0082 167 7E01121 94 7202668 39 7208221 43 PHO0088 194 7E01205 90 92 7 Z02680 51 7208222 44 PHOO090 194 7E01206 90 92 740263953 34 7208226 44 76 78 PH00091 194 701217 101 7202687 28 7Z08227 44 76 78 PH00092 194 7E06031A ii 7202688 38 7208229 44 76 78 PH00093 194 7E06031D 7 7 7202689 38 1208230 44 PH00094 194 7E10039 103 7202692 30 7208238 44 PH00095 194 7E14007 90 92 103 7202693 31 7Z08265 44 PH00096 191 7F01235A 44 77 7202695 31 7208267 76 PH00097 191 7Z01200 87 102 7202696 30 7208268 77 PH00098 191 7Z01201 87 102 7202699 32 7208269 76 PHOO099 191 7Z01202 87 102 7Z02702 4 7Z08270 76 PHO0100 191 7Z01203 87 102 7Z02705 41 7208272 77 96 PHOO101 191 7Z01250 87 101 7Z02706 4 708273 77 PH00102 191 7Z01300 87 103 72027215 32
137. 7Z08275 76 PH00103 191 7201500 86 96 7202722 33 7Z11010 44 PH00104 191 7Z01550 86 92 7202724 33 7Z11200 96 PH00105 191 7Z01560 86 90 7027205 32 7Z14006A 94 PH00106 191 7Z01565 86 98 7Z0272 36 7Z17001 76 PH00107 191 7Z01600 86 94 7202728 36 7Z17200 45 PH00108 191 7Z01601 86 94 7202729 33 717201 45 PH00109 191 7Z02119 40 204 7202730 32 JZAI202 45 PHOO1 10 191 7Z02210 43 2027315 36 PH00015 165 PH00111 191 7Z02212 43 7202733 36 PH00017 165 PH00112 191 7Z02213 43 7202734 37 PH00018 165 PH00113 191 7Z02255 40 7202735 37 PH00019 165 PH00114 191 7202273 30 7202737 32 PH00020 165 PH00115 191 7202402 23 7202738 31 PH00022 165 PH00116 191 7Z02403 27 7202739 37 PH00023 165 PH00117 191 7202404 2 7Z02740 31 PH00024 166 PH00118 191 7Z02405 26 7202741 36 PH00025 166 200 PH00119 191 7202406 26 7202742 28 PHO0026 166 200 PH00120 191 7202410 22 7202743 35 PH00027 200 PH00121 191 Q OPHIR Spiricon Photon 01 08 2013 OPHIR Photonics OPHIR Photonics Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand En Corporation Brand A Newport Corporation Brand A Newport Corporation Brand
138. 8 High Power Applications 199 AN High Power NanoScan 199 Dae High Power Laser Profiler Kits for Nd YAG 201 200 High Power Laser Profiler Kits for CO2 202 3 8 4 High Power ModeCheck A New Method to Assure the Performance of High Power CO Lasers 203 3 8 5 High Power In Line Industrial Beam Monitorin 205 aos VI CO gt Series 205 3 9 Goniometric Radiometers 206 Product Index 211 Part Number Index 220 Distributors list 277 QO OPHIR Spiricon Photon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics 2 OPHIR Photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand A Newport Corporation Brand About Ophir Optronics Ophir Optronics a Newport corporation brand was founded in 1976 as an optical coating company that has grown and diversified into other areas Ophir employs a highly qualified staff of over 570 engineers technicians and skilled workers Our company products are sold worldwide through a distribution network that includes four fully certified calibration facilities and repair centers The majority of Ophir s laser measuring instrumentation line is exported and marketed by sales representatives in more than 35 countries around the world the largest markets being the USA Europe and Japan About Newport Newport was established 45 years ago to create and manufacture solutions to support a newly fo
139. 80 D OPHIR Spiricon 01 08 2013 __ Photonics For latest updates please visit our website www ophiropt com photonics eee Photonics A Newport Corporation Brand A Newport Corporation Brand 3 4 7 Imaging UV lasers Integral Reimaging UV Image Converters The UV image converters are fluorescent plates that convert UV radiation that is poorly imaged by silicon cameras into visible light that is then imaged onto the CCD of the camera These fluorescent plates are specially designed for UV conversion and have a high light output wide linear dynamic range and high damage threshold There are 3 versions available 1 The 4X UV image converter for large beams converts to visible and then images onto the CCD while reducing the beam size 4X 2 The 1 1 UV image converter converts to visible and images the beam onto the CCD without changing the size Jng Shown here is a profile of a 248mm Excimer laser beam 3 The 4X expander with UV converter converts to visible and images a beam enlarged 4X onto the CCD All of the above imagers allow a beam splitter to be mounted at 45 deg angle in front of the imager so as to allow imaging of higher 4X beam reducing UV 1X UV Image 4X beam expander Image Converter as Converter with UV converter power energy beams mounted on camera with Optional Beam Splitter Cross section of 4X reducing UV image Converter A iy N i Y Fluorescent plate Imaging optics Image plane at CCD DN a0 Sp
140. 83040 oO E Measurement CEL ESSW Menu Track parameters Laser lt 8u Average NONE Power measurement Position and size graph Position and size measurement Soft Keys Pointing Stability Screen of Vega Time elapsed since start of measurement Number of position measurement Graphical presentation of all the measurements Marker at point of last measurement Last measurement Statistics since start of measurement Change rate of Reset statistics measurement and graph OU OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Bran 1 2 4 BeamTrack Power Position Size Sensors PC Software Support StarLab COM Object for System Integrators including demo applications in VB VC and MatLab the Track screen to measure power position and size simultaneously m LabVIEW Demo Application Examples of some StarLab Screens 1 2 4 REALL Stability Screen Log data for ia Slee Seer ees ee a eo ee a future review Power measurement and statistics Functions apply to power only Statistics of the stability sample Position amp SizeScreen Bes See j be eee ee es eee eee Se Yoo 7 E F tig E Parameter configuration Functions applies to power only Position and size displayed numerically Graph controls including Sample size Autoscale option Reset but
141. 89 205 PH00404 166 SP90195 156 173 SPZ08234 172 PH00190 205 PH00405 166 SP90197 133 SPZ08235 172 PH00191 205 PH00406 166 SP90198 133 SPZ08240 172 179 PH00192 205 PH00407 166 SP90199 133 SPZ08242 172 PH00193 205 PH00409 166 SP90200 133 SPZ08246 172 PH00198 210 PH00410 166 SP90202D 133 SPZ08253 172 PH00199 210 PH00411 166 SP90202L 133 SPZ08255 198 PHOO200 210 PHO0412 166 SP90203D 133 SPZ08257 178 PHOO201 210 PH00413 166 SP90203L 133 SPZ08259 178 PH00202 210 PH00416 166 SP90204 134 SPZ08260 178 PH00203 210 PH00417 166 SP90205 134 SPZ08261 178 PH00204 210 PH00418 166 SP90207 134 SPZ17005 134 139 PH00205 210 PH00419 166 SP90208 154 SPZ17007 181 PHOO206 210 PHO00420 166 SP90210 134 SPZI7012 172 PH00207 210 PH00439 205 SP90211 204 SPZ17015 177 181 PHOO208 210 SP90038 180 SP90212 204 SPZ17017 179 PH00209 210 SP90057 174 SP90213 204 SPZ17019 178 181 PH00210 210 SP90058 174 SP90219 134 139 SPZ17022 178 PHOO21 1 210 SP90059 174 SP90224 204 SPZ17023 181 PHOO212 210 SP90060 134 SP90227 204 SPZ17024 181 PH00213 210 SP90061 174 SP90228 172 SPZ17025 177 PH00214 210 SP90062 205 SP90229 134 139 SPZ17026 177 178 PH00215 210 SP90075 202 SP90230 134 139 SPZ17027 178 PHOO216 210 SP90076 202 SP90231 134 SPZ17029 174 179 PH00217 210 SP90077 202 SP90232 134 PH00218 194 SP90078 202 SP90233 134 PH00224 194 SP90081 172 SP90234 134 PH00228 166 200 SP90082 181 SP90235 134 PH00229 185 SP90083 181 SP90236 133 PH00230 185 SP90085 180 SP90237 133 PH00231 185 SP90090 154 S
142. 91 NIR500 PH00115 191 NIR750 PH00116 191 NIR1000 PH00117 191 NIST Reference Standard PH00188 208 Nova 7Z01500 86 96 Nova II 7201550 86 92 Nova PE C Adapter 7208272 77 96 Nova RS232 Assembly 2m cable 78105 96 99 Nova RS232 Assembly 5m cable 781052 96 99 NS USB PH00030 166 NS YE PH00050 167 NSEC PH00252 167 NSv1 to NSv2 PRO Upgrade PH00419 166 NSv1 to NSv2 STD Upgrade PH00418 166 NSv2 STD to NSv2 PRO Upgrade PH00417 166 Optical Trigger for FX and SP Cameras SPZ17005 134 139 Option to Fiber Mount BF Ribbon PH00193 208 Optional Mount of User Device LD 8900 Mount PH00181 208 Optional PC oscilloscope SPE10008 198 P200 Power Option PH00046 146 PCI Controller Upgrade PH00187 208 PCI Express FireWire 1394a b Desktop Card SP90164 134 PD10 C 7202944 65 PD10 IR pJ C 7202946 65 PD10 pJ C 7Z02945 65 PD300 7Z02410 22 PD300 F O Adapter FC FC APC type 7Z02213 43 PD300 F O Adapter SC type 7Z08221 43 PD300 F O Adapter SMA type 7Z02212 43 PD300 F O Adapter ST type 7Z02210 43 PD300 1W 7ZO2411A 22 PD300 3W 7202426 22 PD300 BB 7202405 26 PD300 BB 50mW 7Z02440 26 PD300 CDRH 7Z02418 43 PD300 CIE 7Z02406 26 PD300 IR 7Z02412 23 PD300 IRG 7ZO2402 23 PD300 IRG F O Adapter FC FC APC type 7708216 44 PD300 IRG F O Adapter SMA type 7Z08222 44 PD300R 7202436 25 PD300R 3W 7202437 25 PD300R IR 7202439 25 PD300R UV 7202438 25 PD300 StarLink 787100 22 42 PD300 TP 7Z02424 22 PD300 UV 7202413 23 PE9 C 7202933 66 PE9 F 7Z02882 59 PE10BF C 7202938 66
143. A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand NanoScan Options and Accessories Item Description P N P200 Power Option 200mMW maximum power level relative power meter option for Silicon or Germanium detector PH00046 NanoScans The P200 provides better than 1 5 accuracy when calibrated against user s NIST traceable power meter and used in similar input geometry as calibrated Not applicable to Pyro electric detector scan heads NOTE P200 must be specified at time of purchase Can be returned for upgrading NSEC Side exit cable option for NanoScan PHO0252 Cable x Custom NanoScan cable length x PH00049 NS YE Extension NanoScan cable 3m PH00050 C Mnt C Mount attachment for NS PH00051 COL FXT 250 250 mm FL collimation fixture PH00070 PFSA UV Grade fused silica right angle prism front surface attenuator in C mount housing Provides 4 front PH00052 surface reflection DPFSA Dual prism front surface attenuator comprising two UV Grade Fused silica right angle prism units PHO0053 configured orthogonally to preserve polarization in a C mount housing COLFXT 250 TEL X 250 mm FL collimation fixture 1550nm PH00071 COL FXT CO2 Collimation Fixture for 10 6umWL PHO0072 RAL FXT Rayleigh fixture for manual M2 PH00073 RSP100 RailScan motion stage 100mm length PH00078 RSP200 RailScan motion stage 200mm length PH00079 RSP500 RailScan motion stage 500mm length PH00080 H I LA Modify H I for Large 100m
144. Beam Cube Beam Profiling Power Focus Spot Position Temporal Pulse Shape Features Monitor all important beam parameters to keep tight control over process m Beam Cube measures beam profile focal spot position temporal pulse shape and power up to 150W m Portable can be moved from laser to laser to monitor all lasers in plant For measuring at or near focal spot Beam Cube o Atenaiy Adjusimeri Rods 3 7 1 ERMEE 4x 144 20 UNC x 6 5 deep min On Base Plate m2 15 150 REF View A Variab e Filters 4x OF Hole x 2 deeg a On Base Plate Cover Y OPHIR Spiricon Se lL For latest updates please visit our website www ophiropt com photonics go nae 01 08 2013 A Newport Corporation Brand ration Brai A Newport Corporation Brau An integrated laser beam measurement profier system for pulsed and CW lasers System contains an SP620 camera with variable attenuator for beam profiling A thermopile power head for power measurement anda high speed photodiode for temporal pulse width measurement Includes BeamGage Standard beam profiling software and a USBI power meter w StarLab software An optional USB digital oscilloscope is available for temporal measurement of pulsed lasers order p n SPE10008 Or a standard laboratory oscilloscope can be used Diagnostic Capabilities Spatial Beam Profile The Beam Cube shows you the intensity profile of your beam in real time and allows you to
145. C series of pyroelectric sensors m Single shot energy measurement with thermal sensors Optional RS232 interface with Starcom PC application and LabVIEW driver see pages 107 109 m Power and energy logging with graphical display and statistics m Power averaging m Easy to use soft keys menu driven m Screen graphics m Backlight and rechargeable battery m Analog output RS232 cable for Nova m EMI rejection Compatible with the complete range of Ophir thermal power and energy pyroelectric and photodiode sensors Nova is truly versatile measuring power or energy from pJ and pW to hundreds of Joules and thousands of Watts With the optional scope adapter you can connect your pyro sensor to an oscilloscope and see every pulse up to the maximum frequency permitted by the sensor Smart connector sensors automatically configure and calibrate Nova when plugged in Soft keys guide you through the screen graphics Finished working Your configuration can be saved for future use Nova s exclusive autoranging tune screen displays laser power graphically and displays maximum power Zoom and time scale can be adjusted by user 1 4 ERONGA VGK The optional RS232 interface and StarCom PC software allow on line processing of data or processing previously stored data results are displayed graphically on a PC To support PC interfacing LabVIEW drivers are provided 153 00 Poe StarCom Software LabVI EW Selected Screens Digital
146. Cooled Thermal Sensors 150mW to 500W Features FL250A BB 50 FL500A High powers and energies large apertures FL400A BB 50 FL500A LP1 Fan cooled FL400A LP 50 Up to 500W A 50mm and 65mm apertures ed N LN N Model FL250A BB 50 FL400A BB 50 FL400A LP 50 FL500A FL500A LP1 Use General purpose General purpose High power densities Very large aperture High power densities and long pulses and long pulses Absorber Type Broadband Broadband R Broadband RI Spectral Range um 0 19 20 0 19 20 0 4 1 5 10 6 0 19 20 0 25 2 2 Aperture mm p 50MM p 50mm p 50mm 65mm p 65mm Power Mode Power Range 150mW 250W 300mW 400W 300mW 400W 500mW 500W 500mW 500W Power Scales 250W 30W 400W 50W 400W 50W 500W 50W 500W 50W Power Noise Level 10mW 40mW 40mW 25mW 25mW Maximum Average Power Density kW cm2 10 at 250W 12 at 150W 8at400W 12at150W 10at400W 14 at 150W 7at500W 12at150W 16 at500W 39 at 150W Response Time with Meter 0 95 typ s 2 5 2 8 2 8 2 8 2 8 Power Accuracy 3 3 3 3 30 Linearity with Power 1 1 5 1 5 1 5 Re Energy Mode Energy Range 80m4J 300J 75mJ 600J 75mJ 600J 100mJ 600J 100mJ 600J Energy Scales 300J 30J 3J 600J 60J 6J 600J 60J 6J 600J 60J 6J 600J 60J 6J Minimum Energy mJ 80 75 75 100 100 Maximum Energy Density J
147. Corporation Brand 3 4 6 CCTV lens for front imaging through glass or reflected surface When direct imaging in front of the camera for example an image projected onto a diffusing surface such as a ground glass plate it is necessary to reduce the image so that it completely fits onto the CCD chip surface The 25mm and 50mm CCTV lenses image an object from a given plane in front of the lens onto the CCD while reducing the size The lens can image such objects at distances from about 10cm in front of the Spacers lens 20cm for the 50mm lens to 1 meter or more depending on the distance from Focus adj Iris adj the lens to the camera The distance from lens to camera depends on the camera eas type and spacers placed between the lens and the camera Body CCTV Lens Front of camera Camera A Total length of spacers added to system B Detector to Lens spacing Distance A plus the CCD inset for the camera type C Lens to Object spacing Laser Beam CCD inset for Camera Types C mount Camera front to CCD 17 5mm for nominal lens magnification use without spacers CS mount Camera front to CCD 12 5mm for nominal lens magnification use 5mm spacer SP mount SP cameras Camera front to CCD 4 5mm for nominal lens magnification use with 13mm spacers Diffusing glass Object distance vs lens spacing Size reduction vs lens spacing 25mm lens amp 50mm lens E 25mm lens 0
148. D1 filter and 2 ND2 filters are supplied standard with each camera Model Stackable LBF 50 Continuously ATP K Variable UV ND Filters Speciality Filter Speciality Filter ND Filters Variable Attenuator for 355nm for 1300nm ND1 ND2 ND3 Nominal ND value 1 2 3 0 3 0 7 1 2 3 4 1 6continuously ND 1 7 4 6 03 07 10 1 3 Pass 355Nnm Pass 1300nm variable MEAND W7720 23727 blocks 532nm amp blocks lt 1100nm fixed 2 8 gray 30 33 37 40 1064nm glass attenuator 4 3 4 7 5 0 6 0 Clear aperature 19mm O12mm O20mm O15mm O20mm O19mmM 19mm Damage 5W cm 5W cm 5W cm 100mW mm 100W cm2 CW 5W cm 5W cm threshold no distortion no distortion no distortion no thermal 10ns pulses no no distortion no distortion lensing distortion Mounting C Mount Threads C MountThreads C Mount Threads C Mount Threads C Mount Threads C MountThreads C Mount Threads Stackable ND filters The individual filters come in three versions the ND1 filter in the red housing with 10 transmission in the visible the ND2 filter in the black housing with 1 transmission and the ND3 filter in the green housing with 0 1 transmission The individual filters can be screwed on top of each other and thus stacked They are set at a small wedge angle in the housing so as not to cause interference effects ND1 ND2 and ND3 stackable filters Stackable filter LBF 50 showing wedge The LBF 50 comes with a set of filters that are inserted into the flange shown mounted on
149. DIF 33 Features General purpose and high damage threshold a Fan cooled Up to 250W Cc 17 5mm to 35mmM apertures a9 N LA Model F100A PF DIF 18 F150A BB 26 FL250A BB 35 FL250A LP1 35 FL250A LP1 DIF 33 N F100A PF DIF 33 TEs Use Short pulse lasers General purpose General purpose High power density Diffuser for highest and long pulse lasers energy densities paa Absorber Type PF type diffuser Broadband Broadband LP1 LP1 diffuser Spectral Range um 0 24 2 2 0 19 20 0 19 20 0 25 2 2 0 4 3 Aperture mm p 17 5MM Q 33MM p 26mm p 35MM p 35MM p 33MM Power Mode Power Range 50mW 100W 50mW 150W 150mW 250W 150mW 250W 400mW 250W Power Scales 100W 30W 3W 150W 30W 3W 250W 30W 250W 30W 250W 30W Power Noise Level 6mW 3mW 15mW 15mW 20mW Maximum Average Power Density kKW cm 0 5 12at 150W 17 at50W 10 at250W 12 at 150W 27 at 250W 39 at I50W 2 Response Time with Meter 0 95 typ s 2 2 5 lo 2 2 23 Power Accuracy 5 J 3 ck 3 b Linearity with Power 1 5 1 1 1 15 Energy Mode Energy Range 60mJ 200J 20mJ 100J 50mJ 300J 50mJ 300J 400mJ 600J Energy Scales AKO 30J 3J NOG 30 7 337 300i B0070 300J 30J 3J 600J 60J Minimum Energy mJ 60 20 50 50 400 Maximum Energy Density J cm lt 100ns 4 0 3 0 3 0 05 0 5 0 5ms la 5 5 20 200 2MS 3 10 10 50 400 10ms 50 30 30 250 1000 Cooling fan fan fan fan fan Fiber Adapters Available see page 44 NA ST FC SMA SC ST FC SMA SC ST FC SMA SC NA Wei
150. EM Energy Sensor Solutions 84 2 0 Power Meters 85 Power Meter Finder 86 Power Meters and PC Interfaces 88 2 1 Power Meters 89 Aa Vega 89 2a Nova 91 213 LaserStar J3 2 1 4 Nova 95 FAN StarLite me 2 1 6 Accessories 99 PC Connectivity Options for Power Energy Measurement 100 Table of contents Page 2 OPHIR Spiricon Photon Photonics For latest updates please visit our website www ophiropt com photonics 2 OPHIR Photonics OPHIR Photonics A Newport Corporation Brand A Newport Corporation Brand A Newport Corporation Brand 1 0 BStelaiseyes 2 0 Ben ielaileitelas 3 0 MSRM IOE 1 01 08 2013 2 2 PC Interfaces 101 22 1 Compact Juno USB Interface 101 220 Pulsar Multichannel and Triggered USB Interfaces 102 243 Quasar Wireless Bluetooth Interface 103 Summary of Computer Options for Ophir Meters and Interfaces 104 2 3 Software Solutions 105 23 1 StarLab 105 2 3 2 Starcom 107 7 254 LabVIEW Solutions 109 2 4 OEM Power Meter Solutions 110 O 24 1 Examples of Custom OEM Power Energy Meter Solutions 110 7 3 0 Laser Beam Analysis 111 Ca 3 1 Choosing a Beam Profiler 112 311 Four Basic Questions ee oe O gt 1 One More Question 113 e or ie User Guide for Choosing the Optimum Beam Profiling System 114 AN Benefits of Beam Profiling 116 3 2 Introdu
151. Energy Range Page F100A PF DIF 18 High average power short pulse lasers O17 5mm 0 24 2 2uM 50mW 100W 60mJ 2005 36 F100A PF DIF 33 As above aperture 33mm 033mm 0 24 2 2UM 50mW 100W 60mJ 2005 36 F150A BB 26 Fan cooled to 150W O26mmM 0 19 20UmM 50mW 150W 20mJ 100J 36 FL250A BB 35 Fan cooled to 250W O35mm 0 19 20uUm 150mW 250W 50mJ 300J 36 FL250A LP1 35 As above high damage threshold for long pulses and CW 35mm 0 25 2 2uM 150mW 250W 50mJ 300J 36 FL250A LP1 DIF 33 Fan cooled to 250W with diffuser for high powerand 33mm 0 4 3um 400mW 250W 400m4J 600J 36 energy density FL250A BB 50 Fan cooled to 250W large aperture O50mm 0 19 20uUm 150mW 250W 80m4J 300J af FL400A BB 50 Fan cooled to 400W O50mm 0 19 20um 300mW 400W 75mJ 600J 37 FL400A LP 50 Fan cooled to 400W high power densities and long pulses 50mm 0 4 1 5um 10 6um 300mMW 400W 75mJ 600J 37 FL500A Fan cooled to 500W very large aperture O65mm 0 19 20UmM 500mW 500W 100mJ 600J a7 FL500A LP1 Fan cooled to 500W high power densities and long pulses 65mm 0 25 2 2UM 500mW 500W 100mJ 600J 37 High power water cooled thermal sensors and power pucks 1W 10kW Sensor Features Aperture Spectral Range Power Range Energy Range Page L250W Thin profile 20mm thick water cooled to 250W 50MM 0 19 20um 1W 250W 120mJ 200J 38 L300W LP Thin profile 20mm thick water cooled to 300W O50mm 0 4 1 5um 10 6um 4W 300W 200m4J 300J 38 1000W Water cooled to 1000W 34Mm 0 19 20um 5W 1000W 300mJ 300J 39 1000W LP Water cooled to
152. Il VI CO2 58 Top View De Ss E Se Geet TE j sH I F Cee an As AE i j f ee mi oe p Hi n KA E roe hs n Ta X ca md a aa re s f a Sen RS O Be yee Ga II VI CO 58 D8 WC V seni lt Side View bs aj c cma YU F agp aa Tan iasan e ak Pom s or Races aie 0 0 i E t M Model Wavelength Power Beam Width Beam Input Cooling IMCO BS o 10 6um up to 8kW 20mm Vertical or Horizontal Requires external water II VI CO gt 58 D8 WC H 10 6um up to 10kW 29mm Horizontal Requires external water lI VI CO gt 58 D8 WC V 10 6um up to 10kW 29mm Vertical Requires external water Ordering Information Item Description P N I VI CO2 BS 35 Il VI CO in line sampler for 10 6um beams up to 8 kW Beam width up 20 mm Pyrocam Ill Beam Profiler System SP90062 required ordered separately Recommended model PY III C A or PY III C B with a Germanium 10 6um window BGS PC PIll laser beam analyzer software included with Pyrocam system II VI CO gt 58 D8 WC H CO laser beam sampler for lasers up to 10kW Input Clear Aperture is 58mm Requires cooling water Horizontal SP90160 entry Built in 8X beam reducer and adapters for Pyrocam Ill Order Pyrocam Ill separately BGS PC PIll laser beam analyzer software included with Pyrocam system I VI CO gt 58 D8 WC V Same as above but with Vertical Entry SP90161 Y OPHIR Spiricon gt Photonics For latest updates please visit our website www ophiropt com photonics
153. Laser Power amp Energy Measurement Laser Beam Analysis 2013 OPHIR Spiricon Photon Photonics OPHIR Photonics OPHIR Photonics A Newport Corporation Brand A Newport Corporation Brand A Newport Corporation Brand Ophir now part of the Newport Corporation Family of Brands Ophir Photonics Group For Every Laser Measurement United to Lead the Industry For over 35 years Ophir has met the challenge to consistently provide accurate and reliable laser power and energy measurement devices Spiricon and Photon during that time have established themselves as the leader in beam profiling Our first class teams of scientists and engineers set the standard for innovation in the face of increasing demands for durability and precision The Ophir Photonics group leads the industry in all aspects of laser beam measurement Continual Improvement Improvements in material science continually extend the operational limits of our increasingly damage resistant laser measurement devices This not only ensures our undisputed position at the forefront of laser measurement technology but also confirms our commitment to you in providing the most accurate and durable products in the market Constant attention to improved calibration methods further solidifies our leadership position in reliable and accurate instrumentation As an ISO 9001 2008 company we subject our products and systems to constant quality assurance monitoring We are also pr
154. MOUNTING THREADS 2 SIDES C 2x M3x5deep MOUNTING THREADS 2 SIDES SHIELDED CABLE TO OPHIR SMART CONNECTOR 50 OU OPHIR 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 1 1 5 1 Standard OEM Thermal Sensors 60mW to 100W Features Conduction or water cooled Spectrally flat m UA version can give analog voltage output or digital RS232 output and can measure power Can also have multiple switchable ranges and or multiple switchable wavelengths 100C SH m UAU version is similar to the UA version but operates via the USB terminal of the PC The following specifications refer to standard OEM sensors and are to be understood as generic describing sensor families Ophir will be happy to help you with a specific solution for your particular application 100C UA 100C UAU Model 100C SH 100C UA 100C UAU Type Smart sensor Digital RS232 connection Digital USB connection analog or digital output digital output Features Low profile smart sensor Low profile separate amplifier Low profile separate amplifier Absorber Type Broadband Broadband Broadband Spectral Range um 0 19 20 0 19 20 0 19 20 Aperture mm 018 018 018 Power Mode Maximum power 100W if used with suitable heat sink 4W free standing 100W if used with suitable heat sink 4W free standing 100W if used with suitable heat sink
155. NA 7 350 400 NA 3 400 950 5 430 950 3 400 950 5 430 950 3 400 950 5 430 950 3 400 950 5 400 950 5 950 1100 7 950 1100 5 950 1100 7 950 1100 5 950 1100 7 950 1100 5 950 1100 7 950 1100 Damage Threshold W cm 10 50 10 10 10 100 10 50 Max Pulse Energy uJ 2 20 2 100 20 500 1 100 Noise Level for filter out pW 20 20 200 2 Response Time with Meters 0 2 0 2 0 2 0 2 Beam Position Dependence 2 2 2 3 nA Background Subtraction 95 98 of background is cancelled automatically under normal NA NA room conditions even when changing continuously Fiber Adapters Available SMA FC ST SC SMA FC ST SC SMA FC ST SC NA see page 43 Version V1 Part Number Standard Sensor 7Z02410 7Z02411A 7Z02426 7Z02424 StarLink Sensor Direct USB 787100 link to PC p 42 Note a Maximum power density For graphs see page 24 For PD300 3W drawing see PD300 UV PD300 IR drawing in page 23 PD300 PD300 1W filter installed PD300 PD300 1W filter off PD300 TP 119 5 S 118 96 Zi 40 5 65 32 i F T gw a e E ERs Bottom View a an Bottom View Front View Front View FILTER IN FILTER OUT 01 08 2013 AA OPHIR Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 1 1 1 1 Standard Photodio
156. OPHIR Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand a Corporation Brand y e ks h Wireless Interface PC Interfaces Quasar Juno USBI Pulsar 4 Pulsar 2 Pulsar 1 N A N A N A N A N A N A N A N A N A N A N A N A N A N A N A N A N A N A Yes Powered from USB Powered from USB No No No Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes No No Yes No No No No Yes No No No No Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes Yes No No 1V No No No No No No Yes Yes Yes N A N A N A N A N A N A N A N A N A N A N A N A N A 10 000Hz 2000Hz 25 000Hz 25 000Hz 25 000Hz 500Hz N A N A N A N A N A No No No No No No No Yes Yes Yes Yes Yes No Yes Yes Yes Yes Yes 7Z01300 7Z01250 7Z01200 7Z01201 7Z01202 7Z01203 103 101 102 102 102 Q OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand 2 0 EROAA VARE 87 For latest updates please visit our website www ophiropt com photonics 01 08 2013 Power Meters and PC Interfaces Ophir power meters and PC interfaces work on the smart plug principle This means that almost any Ophir power meter or PC interface can work plug and play with almost any of the wide range of Ophir sensors Ophir power meters are also the most sensitive lowest noise Most precise calibration units on the market thus giving the untmos
157. OUNTING THREAD 35 VIEW A 1 9 5 ss 6 8 J Molex 6 Pin 35 4x M3x5 MOUNTING THREAD SK Male Header Q OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics N N U N uan af 51 01 08 2013 1 1 5 1 Standard OEM Thermal Sensors 60mW to 150W Features 150C SH 150C UA 150C UAU 150W UA 150W UAU Conduction or water cooled Spectrally flat m UA version can give analog voltage output or digital RS232 output and can measure power or energy Can also have multiple switchable ranges and or multiple switchable wavelengths m UAU version is similar to the UA version but operates via the USB terminal of the PC The following specifications refer to standard OEM sensors and are to be understood as generic describing sensor families Ophir will be happy to help you with a specific solution for your particular application 1 1 5 1 Qfelawteras Model 150C SH 150C UA 150W UA 150C W UAU Type Smart sensor Digital RS232 connection Digital RS232 connection Same as UA but with digital analog or digital output analog or digital
158. P90238 133 PH00232 185 SP90091 154 SP90239 133 PH00233 194 SP90092 154 SP90241 133 PH00234 194 SP90093 154 SP90242D 133 PH00235 194 SP90101 154 SP90242L 133 PH00236 194 SP90102 154 SP90243D 133 PH00237 194 SP90103 154 SP90243L 133 PH00238 194 SP90104 154 SP90246 133 PH00239 194 SP90105 154 SP90247 133 PHOO240 194 SP90106 154 SP90248 133 PH00241 194 SP90107 154 SP90249 133 PHO0242 194 SP90108 154 SP9025 1 133 zia p 2al Q OPHIR Spiricon Photon OPHIR Photonics OPHIR Photonics 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand A Newport Corporation Brand Ophir Photonics sites Country Company Telephone E mail USA Ophir Spiricon LLC 435 753 3729 sales us ophiropt com Japan Ophir Japan 81 48 646 4150 info ophirjapan co jp Israel Ophir Optronics Ltd 972 2 5484444 sales ophiropt com or anatd ophiropt com Germany Ophir Spiricon Europe 49 4102 667 1 802 juergen reingruber eu ophiropt com Distributors list Ophir Ophir Ophir Photonics Spiricon Photon Country Company Telephone E mail Power Beam Beam Meters Profilers Profilers Australia amp N Z a Applications 612 9979 7646 johng raymax com au 5 Nn YAA a gg Australia amp N Z Warsash Scientific 612 9319 0122 sales warsash com au Austria Ophir Spiricon Europe 49 4
159. PD300 TP Mounted on stand Features Ta m Very large dynamic range O Swivel mount for hard to measure places N Comes with filter in filter out options Patented automatic background subtraction Ca Fiber optic adapters available m Model PD300 PD300 1W PD300 3W PD300 TP po Use General Powers to 1W Powers to 3W Thin profile for tight fit Detector Type silicon silicon silicon Silicon Aperture 10x10mm 10x10mm 10x10mm 10x10mm Filter mode Filter out Filter in Filter out Filter in Filter out Filter in Filter out Filter in Spectral Range nm 350 1100 430 1100 350 1100 430 1100 350 1100 430 1100 350 1100 400 1100 Power Range 30mW to 500pW 300mW to 30mW to IW to 200 uW 100mW to 5nW 3Wto200uW 3mW to50pW 1W to 20uW 200uW 500pW Power Scales 30mW to 30nW 300mW to 30mW to 30nW 1W to 30mW 100mW to 3Wto30mW 3mWto3nW 1Wto3mW and dBm 30mW and dBm and dBm and dBm 300nW and dBm and dBm and dBm and dBm Resolution nW 0 01 NA 0 01 NA 0 1 NA 0 001 1 Maximum Power vs nm mW mW nm mW mW nm mW mW nm mW mW Wavelength lt 488 30 300 lt 488 30 1000 lt 488 100 3000 350 3 NA 400 633 20 300 633 20 1000 633 100 3000 400 3 1000 500 670 13 200 6 0 13 1000 670 100 2000 600 2 5 1000 790 10 100 790 10 600 790 100 1200 700 2 500 904 10 100 904 10 700 904 100 1200 800 1 5 300 950 1064 23 250 1064 25 1000 1064 100 2200 1064 3 500 Accuracy including errors due to temp variations error vs Wavelength nm 10 360 400 NA 10 360 400 NA 10 360 400
160. PH00023 165 USB NS Ge 9 5 STD PH00394 165 USB NS Ge 9 25 PRO PH00022 165 USB NS Ge 9 25 STD PH00393 165 USB NS Ge 1 2 25 PRO PH00024 165 USB NS Ge 12 25 STD PH00395 165 USB NS PYRO 9 5 PH00025 200 USB NS PYRO 9 5 PRO PH00025 166 USB NS PYRO 9 5 STD PH00396 166 USB NS PYRO 9 25 PH00228 200 USB NS PYRO 9 25 PRO PH00228 166 USB NS PYRO 9 25 STD PH00400 166 USB NS PYRO 20 25 PH00026 200 USB NS PYRO 20 25 PRO PH00026 166 USB NS PYRO 20 25 STD PH00397 166 USB NS PYRO HP 9 5 PH00028 200 USB NS PYRO HP 20 10 PH00027 200 USB NS Si 3 5 1 8 PRO PH00015 165 USB NS Si 3 5 1 8 STD PH00386 165 USB NS Si 9 5 PRO PH00018 165 USB NS Si 9 5 STD PH00389 165 USB NS Si 9 25 PRO PH00017 165 USB NS Si 9 25 STD PH00388 165 USB NS Si 25 25 PRO PH00019 165 USB NS Si 25 25 STD PH00390 165 USB Pass Fail Cable SP90060 134 USB to Bluetooth adapter 7E10039 103 USBI 7Z01200 8 UV PHOO212 210 UV converter assembly for 4X beam expander SPZ17019 178 181 UV Lens Kit PH00097 191 UV ND Filters SP90228 172 UV200 PH00098 191 UV250 PH00099 191 UV350 PH00100 191 UV500 PHOO101 191 UV750 PH00102 191 UV1000 PH00103 191 Uview Accessory for C mnt Cameras SP90322 182 Variable filter SPZ1 012 172 Vega 7Z01560 86 90 VIS200 PH00105 191 VIS250 PH00106 191 VIS400 PH00107 191 VIS500 PH00108 191 VIS750 PH00109 191 VIS1000 PH00110 191 WL O PH00183 208 WVF 300 SP90195 156 173 s a i 219 OU OPHIR Spiricon Photon Photonics For latest updates please visit our website w
161. PHIR Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand USB Cameras for use with Laptop or Desktop PC Item Specification Model SP503U SP620U USB L11059 Application Y2 format slim profile wide dynamic 1 1 8 format high resolution wide 36mm x 24mm 35mm format for large Spectral Response Active Area Pixel spacing Number of effective pixels Minimum system dynamic range Linearity with Power Accuracy of beam width Frame rates In 12 bit mode Shutter duration Gain control Trigger Photodiode trigger Saturation intensity Lowest measurable signal Damage threshold Dimensions and CCD recess Image quality at 1064nm Operation mode range CW amp pulsed lasers adjustable ROI 190 1100nm 6 3mm W x 4 7mm H 9 9um x 9 9um 640 x 480 64 dB 1 2 30 fps at full resolution 60 fps at 320x240 30us to multiple frame times 43 1 automatic or manual control dynamic range pulsed lasers CW YAG adjustable ROI 190 1100nm 7 1mm W x 5 4mm H 440um x 4 40um 1600 x 1200 62 dB 1 7 5 fps at full resolution 28 fps at 640x480 44 fos at 320x240 29 1 automatic or manual control 1 BNC connector accepts positive or negative trigger LED on camera indicates triggering Will synchronize with laser repetition rates up to 1KHz Buil
162. PS General purpose Broadband 0 19 20 p 50mm 150mW 250W 250W 30W 15mW 10 at 250W 12 at 150W 2 8 3 1 5 80mJ 300J 30017 3057 3 80 0 3 J 10 30 0 2 0 1 2W 5 for centered beam 5 35 3 W cm fan ST FC SMA SC 0 9 7Z07902 787201 Notes d Assumes laser beam with Gaussian TEM distribution For other modes size measurement is relative Notes e Accuracy spec will be maintained for beams from 6 to 35mm not deviating from center more than 15 of beam diameter FL250A BB 50 PPS Absorber Surface 10 2 18 O DC power supply socket 106 90 2x M3x4 5 deep 58 a S D ADJUSTABLE 107 153 ii lt a Q OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics 1 2 4 BeamTrack Power Position Size Sensors Device Software Support BeamTrack sensors are fully supported by the Vega Nova ll StarLite and Juno devices Attach the sensor to the meter On startup it will be recognized as a BeamTrack sensor and tracking options will be enabled m Use the Track screen to measure power position and size simultaneously 2 Use the Stability screen to measure pointing stability also known as beam wander over time Q DU N N Track Screen on Nova ll Sensor type and S N S0A PPS 9
163. Power Screen 129 1 be CW industrial medical and scientific lasers W pial Laser Units w or dom pW to multi kW with appropriate sensors Bargraph with zoom Press Menu button or soft keys to make legends visible not shown e YAG Laser Laser Tuning Screen or 29 8 Max power Power Log Screen not shown W Units m Maximizing laser power ERIT m User selected time period and zoom Press Menu button or soft keys to make legends visible Time Exit 50 Zoom Sweep Time O OPHIR ee For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand orporatio Energy Measurement Screen 1 1064 Laser m Pyroelectric and thermopile g m ad Units sensors single pulse POWER oor RAHGE Soft key legends Pyroelectric frequency E Change range measurement not shown Change to Power Zoom bar graph Measurement Flashes Ready for next pulse Energy Log Screen 1064 Laser wavelength m Pyroelectric sensors 1 063 Energy of last pulse m Thermopile sensors successive single pulses M m Continuous scroll EXIT m Energy statistics Press Menu button or soft keys to make legends visible not shown N lt Pyroelectric Exposure Screen O m Sum or average energies over 1 PA a Fe mM AE VU user selected time period number 14 5 Sec ees a a gt of pulses STOF RESET EXIT Mea
164. Pucks 5W to 1500W Features m High powers m Water cooled 1000W 1000W LP L1500W L1500W LP Upto 1500W A 034mm and 50mm apertures U N O N Model 1000W 1000W LP L1500W L1500W LP Use General purpose High power densities General purpose High power densities and long pulses and long pulses Absorber Type Broadband P Broadband LP Spectral Range um 0 19 20 0 4 1 5 10 6 0 19 20 0 4 1 5 10 6 Aperture mm p 34mm p 34mm p 50MM p 50mm Power Mode Power Range 5W 1000W 5W 1000W 15W 1500W 15W 1500W Power Scales 1000W 200W 1000W 200W 1500W 300W 1500W 300W Power Noise Level 200mW 200mW 700mW 700mW Maximum Average Power Density kW cm 7 5 at 500W 6at1000W 9at500W 7 at1000W 7 5 at 500W 5at1500W W 9at500W 6at 1500W Response Time with Meter 0 95 typ s 2 5 2 5 2 7 2 7 Power Accuracy 3 3 a 4 fa 4 a Linearity with Power 2 2 2 2 Energy Mode Energy Range 300mJ 300J 300mJ 300J 500mJ 200J 500mJ 200J Energy Scales 300J 30J 3001 30J 200J 20J 200J 205 Minimum Energy mJ 300m4J 300m4J 500m4J 500m4J Maximum Energy Density J cm lt 100ns 0 3 0 05 0 3 0 05 Tus 0 4 0 3 0 4 OB 0 5ms 5 20 5 20 2ms 10 50 10 50 10ms 30 150 30 150 Cooling water water water water Minimum Water Flow Rate at Full Power 1 8 liter min 1 8 liter min 2 5 liter
165. Pyro HP NS Neel 3 3 en IINS 51 275 NS Si 9 5 NS Si 9 5 NS Si 9 5 UV Vis SP620 mere NS Pyro Neer yike 2 oom NSE vie 2 5am Te So 9 oan NS eye 9 5 SP620 SP620 SPO 0 SP620 SP620 NS Pyro HP NS NS Ge 3 5 1 8 NS Ge 9 5 NS Ge 9 5 NS Ge 9 5 NS Ge 9 5 NS Ge SP620 NS Pyro NS Pyro 9 5 NS Pyro 9 5 NS Pyro 9 5 NS Pyro 9 5 NIR 1000 1100nm SP620 SP620 SP620 SP503 Pyrocam NS Ge NS Pyro HP NS NS Ge 3 5 1 8 NS Ge 9 5 NS Ge 9 5 NS Ge 9 5 NS Ge79 5 Eye Safe 1100 1800nm XEVA XEVA XEVA Pyrocam Pyrocam NS Ge NS Ge NS Ge NS Ge 3 5 1 8 NS Ge 9 5 NS Ge 9 5 Pyrocam NS Ge 9 5 1500 1600nm SP 620 1550 SP 620 1550 SP 620 1550 SP 620 1550 XEVA SP 620 1550 XEVA Pyrocam NS Pyro HP NS Pyrocam NS Pyro 9 5 NS Pyro 9 5 NS Pyro 9 3__ NS Pyro 9 5 w Beam Expansion N i MIR amp FIR Pyrocam NS Pyro Pyrocam Pyrocam gt a Pyrocam g z ModeCheck DO ae ae _ Abbreviations FIR Far Infrared NIR Near Infrared Ge Germanium Si Silicon HP High Power SP Indicates camera profiler MIR Mid Infrared NS NanoScan UV Vis Ultraviolet Visible 114 D OF PHIR Spiricon Photon 01 08 2013 a For latest updates please visit our website www ophiropt com photonics 2 OPHIR Photonics e ells A Newport Corporation Brand orporation Bral A Newport Corporation Brand A Newport Corporation Brand Laser Minimum CW or Pulsed Wavelength Beam Size Pulsed Pulsed gt 5mm gt 10mm CW lt 1kHz S1kHz No optics Speed Ease of use NS Ge 12 25 NS SP620
166. RS 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand 3 9 Goniometric Radiometers LD 8900 LD 8900R Far Field Profilers Profiling divergent light sources presents many challenges but Photons far field profilers characterize the angular radiation intensity of light simply and accurately in real time Both the LD 8900 and LD 8900R wide dynamic range Goniometric Radiometer provide full 3 dimensional measurements of the far field pattern in minutes or less with far better resolution than a CCD camera The LD 8900 far field profiler provides direct real time far field measurements with gt 24dB dynamic range while the wide dynamic range LD 8900R has a dynamic range of gt 36dB which provides greater detail in the tails of the far field pattern Both models have an angular sampling resolution of 0 055 and a field of view of 72 144 and are ideal for characterizing the light flux from many sources including VCSELs laser diodes LDs optical fibers optical waveguides and more With the LD 8900R measurement of the mode field diameter of optical fiber is possible in real time with greater than 5 accuracy The LD 8900 and the LD 8900R are available with either a silicon or InGaAs detector and have a standard entrance aperture of 2mm with an optional 10mm entrance aperture for use with larger sources such as LEDs and LD bars LD 8900 and LD 8900R complete systems include The Scan
167. S 7Z02743 7Z02651 Notes a LP1 sensors have relatively large spectral variation in absorption c For 10 50Hz derate as follows b Sensor has a window and have a calibrated spectral curve at all wavelengths in their Wavelength Derate to value for gel coupled IPL sources spectral range to the above specified accuracy Nova and Orion 1064nm Not derated where IPL source is coupled to meters do not support this feature and when used with those 532nm Not derated window with gel or water for meters accuracy will be 3 for 532nm 808nm 1064nm and 355nm 70 of stated value measurement Can also measure 2100nm and 6 for other wavelengths in the spectral range 266nm 15 of stated value air coupled IPLs 400 1100nm 193nm 10 of stated value d Damage threshold 1 5J cm2 for wavelengths lt 500nm L50 300 A L50 300 A LP1 L50 300 A PF 65 L50 300 A IPL 120 30 120 i 36 21 t 1 ADJUSTABLE 122 168 ae t5 100 75 OU OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand 1 1 2 5 Medium High Power Fan Cooled Thermal Sensors 50mW to 250W F100A PF DIF 18 F150A BB 26 FL250A BB 35 FL250A LP1 35 FL250A LP1
168. Scan M Systems USB MSP NS Si 9 5 Model 1740 ModeScan with NanoScan Silicon Si Detector 9mm aperture 5um slits Si detector PH00233 63 5mm diameter head 9mm entrance aperture and matched pair of 5 0um wide slits Use from 190 to 1000nm wavelengths USB MSP NS Ge 9 5 Model 1740 ModeScan with NanoScan Germanium GE Detector 9mm aperture 5 0um slits PHO0234 Germanium detector 63 5mm diameter head 9mm entrance aperture and matched pair of 5 0um wide slits Use from 700nm to 1 8um wavelength USB MSP NS Pyro 9 5 Model 1740 ModeScan with NanoScan Pyroelectric Detector 9 0mm aperture 5um slits Pyroelectric PH00235 detector 63 5mm diameter head 9mm entrance aperture and matched pair of 5um wide slits MSP NS Pyro 20 25 Model 1740 ModeScan with large aperture NanoScan scanhead with 20mm Pyroelectric Detector PH00218 25um slits 100mm diameter head 20mm entrance aperture and matched pair of 25um wide slits USB MSP HPNS 10 5 Model 1740 ModeScan with HP NanoScan scanhead with 9mm Pyroelectric Detector 5um PH00236 slits 100mm diameter head 9 mm entrance aperture and matched pair of 5um wide slits scanhead is N fancooled DN NanoModeScan Accessories oo LENS 200 UV XXX Optional 200mm quartz lens for use between 190 400nm wavelengths PHOO090 LENS 400 UV XXX Optional 400mm quartz lens for use between 190 400nm wavelengths PHO0091 LENS 190 10 6 Optional 7 5 inch focal length lens for use at 10 6um wavelength
169. StarLab softwrare see section 2 3 1 on page 105 Below is a list of the StarLink power sensors currently available together with the reference page for the specifications on the relevant sensor StarLink Sensor StarLink P N Corresponding Ophir P N Data sheet page stand alone sensor PD300 StarLink 787100 PD300 7Z02410 22 3A StarLink 787000 3A 7Z02621 28 3A QUAD StarLink 787203 3A QUAD 7207934 56 3A P StarLink 787001 3A P 7202622 28 3A FS StarLink 787002 3A FS 7202628 28 10A StarLink 787004 10A 7202637 30 10A PPS StarLink 78 202 1OA PPS 7207904 56 30A BB 18 StarLink 787006 30A BB 18 7202692 30 50 150 A BB 26 PPS StarLink 787200 50 150 A BB 26 PPS 7207900 5 7 30 150 A BB 18 StarLink 787007 30 150 A BB 18 7Z02699 32 L50 150 A StarLink 787003 L50 150 A 7202633 34 FL250A BB 50 PPS StarLink 787201 FL250A BB 50 PPS 7Z07902 58 1000W StarLink 787005 1000W 7Z02664 39 01 08 2013 AA OPHIR Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 1 1 4 Power Sensors Accessories 1 1 4 1 Accessories for PD300 Sensors For PD300R PD300 IRG and 3A IS series see page 44 Fiberoptic Adapters PD300 with F O Adapter Mounted Ca ae Y C YU N N q q Accessory Description Part number PD300 CDRH 7mm aperture adapter 7Z02418 for CDRH measurements Fiber Adapters Adapters for mounting SC type ST type FC FC APC type SMA type fibers to PD300 sens
170. T with above fiber adapters gt iy 4 E a SH to BNC adapter ea al Allows raw voltage output from FO ADAPTER ee thermal sensors e L 75 Ta e IR Phosphor Glass lt Q OPHIR 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 1 1 4 3 High Power Water Cooled and Fan Cooled Laser Beam Dumps Up to 10kW Features Upto 10kW CW Water or Fan cooled BDFL500A BB 50 BD5000W BB 50 BD10K W High Power Density 45 50mm aperture U N m Model BDFL500A BB 50 BD5000W BB 50 BD10K W is Use General purpose High power beam dump Absorber Type Broadband Broadband Beam Deflector Broadband Spectral Range um 0 19 20 0 19 20 0 19 20 Typical Absorption 86 for 600 to 2500nm 82 for 10 6um Aperture mm p 50mm p 50mm p 45mm Maximum Incident Power 500W 5000W 10 000W Maximum Average Power Density 7kW crm 6kW cm at 1000W See note b below 3kW cm2 at 5000W Maximum Energy Density J cm See note b below lt 100ns 0 3 1 us 0 4 0 5ms 5 2Ms 10 10ms 30 Cooling Fan water water Minimum Wa
171. Unit a The Motion Control Module Goniometric Radiometer Acquisition and Analysis Software for Microsoft Windows operating systems PCI Interface Box Power and instrument cables An optional semi custom source mount specifically designed to meet your application needs can be quoted upon request for either the LD 8900 or the LD 8900R Mode Field Diameter in Real Time with LD 8900R The LD 8900R allows for real time measurements of Mode Field Diameter MFD with an accuracy of 5 for a nominal 10um single mode fiber Mode Field Diameter MFD of single mode optical fiber is measured using the methodology described in the Telecommunication Industry Association Electronic Industries Association TIA EIA Standard FOTP 191 Specifically the MFD is calculated using the Petermann Il integral with data sampled at angular resolution of 0 055 and collected over an angular extent of 72 144 viewing angle If greater accuracy is required Photon s LD 8900HDR is specifically designed to measure MFD and A to greater than 0 5 E a TF a ty SAn uk OR FAR OO ae e 3 9 EEEN Bs eens oe mi ee pe Windows Showing Unifomity of a Laser Diode ty es in Topographical View LD 8900R Laser Diode Diffraction Rings n Q OPHIR Photon a For latest updates please visit our website www ophiropt com photonics ORE Photonies A Newport Corporation Brand Newport Corporatio A Newport C
172. V J into IMQ at 2 9um Max Pulse Width 300us b Ims Ims 3ms Maximum Pulse Rate pps AQ b 20 20 1000 Frequency Dependence lt 2 to maximum frequency Pulse Width Dependence lt 2 to maximum pulse width Noise Equivalent Energy approx Suu 50uJ 150uJ Output BNC BNC BNC Customer specified Volt J into input impedance of gt 3kQ Output Hold Hold time can be specified by customer Calibration Adjustment Trimpot accessible through back cover of sensor Maximum Energy 10J 10J 10J 10J Minimum Energy 0 1mJ ImJ 3mJ 0 1mJ Damage Threshold J cm lt 100nm 0 1 0 3 2 1 5 Tus 0 2 0 3 a 3 300us 2 1 10 8 100 depending on wavelength Linearity with Energy 2 for gt 10 of full scale Maximum Average Power W 10 10 30 50 Maximum Average Power Density W cm 10 10 300 Dimensions 50 8 x 14mm O50 8 x 14mm 50 8 x 18mm O50 8 x 28mm Part Number Consult Ophir representative Notes a At calibrated wavelength standard 1064nm Others on request Notes b There is a trade off between repetition rate sensitivity and maximum pulse width If standard products are not suitable these parameters can be tailored to customer requirements Notes c XXX denotes the calibration wavelength in um and the YYY denotes the calibrated sensitivity in V J Notes d Output voltage is limited to 1 5 volt less than input V For example if input voltage is 6V and sensitivity is 10V J then maximum pulse energy is limited to 4 5V output of 0 45 Notes e Accura
173. Wedge Additional wedge beam 93mm SPZ17026 Beam Splitter splitter to mount to 1st wedge beam splitter 1 For converging beams a larger aperture 1st beam splitter is available P N SPZ 17025 In that case the aperture at the 1st beam splitter is 30mm Large aperture For converging beams a larger 30mm SPZ17025 1st Wedge aperture 1st wedge beam Beam Splitter splitter Aperture is 30mm Single and Dual Prism Front Surface Beam Samplers With large beam splitter mounted showing how to image The Prism Front Surface Beam Sampler PFSA is a C mount fixture housing a UV Grade Ce ae Fused Silica right angle prism used for sampling the front surface reflection for high power energy beam profiling applications Reflection at nominal incidence of 45 is polarization and wavelength dependent with 532nm s polarization reflected at 8 27 and p polarization at 0 68 The system is available as either a single prism PFSA or dual orthogonal prism DPFSA unit The dual orthogonal prism configuration results in polarization independent reflection of 0 057 at 532nm Other filters and attenuators can be attached using the C mount female threads at the input end The use of a right angle prism to sample the incident beam guarantees that any scattered secondary beams do not interfere with measurement as shown in the sketch Reflected Beam Dual Prism Front Surface Sampler Y N Ca Incident Beam O lt Scattered Beams on Pris
174. X 6 5 14 CONNECTOR FRONT VIEW SIDE VIEW REAR VIEW 38 2 SIDES 28 A 65 14 38 2 SIDES 28 38 i AE 5 5 MOUNTING HOLES 38 Oot 28 2x M4x7deep MOUNTING HOLES MOUNTING HOLE PONa A RIDER 4x M4x4deep C a MOUNTING HOLES 8 32 UNC 2 SIDES 4x M4x4deep FOR MOUNTING ROD MOUNTING HOLES G 32 UNC FOR MOUNTING ROD EE BETER REAR VIEW SIDE VIEW FRONT VIEW SMART CONNECTOR Q OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 1 1 5 1 Standard OEM Thermal Sensors 8OmW to 50W Features L30C SH L30C UA Conduction cooled Spectrally flat 2 m UA version can give analog voltage output or digital RS232 output and can measure power or energy Cc Can also have multiple switchable ranges and or ap multiple switchable wavelengths Y m UAU version is similar to the UA version but operates via the USB terminal of the PC Lr These specifications refer to standard OEM sensors and are to be understood as generic describing sensor families Ophir will be happy to a help you with a specific solution for your particular application q Model L30C SH L30C UA L30C UAU Type Smart sensor Digital RS232 connection Digital USB connection analog or digital output digital output Features Medium aperture smart sensor Medium aperture built in Medium aperture built in amplifier amplifier Absorber Type Broadband Broadband Broadband
175. XT 250 PHOO070 167 COL FXT 250 TEL X PH00071 167 COL FXT CO2 PH00072 167 Comet 1K 7 Z02702 41 Comet 10K 7202705 41 Comet 10K HD 7 Z02706 41 CUSTOM LENS PH00088 194 Damage Threshold Test Plates BF type 7E06031D 76 Damage Threshold Test Plates Metalic type 7E06031A 76 DPFSA PH00053 167 Extended Cable Option EXT Cable PH00184 208 F100A PF DIF 18 7202741 36 F100A PF DIF 33 7 Z02744 36 F150A BB 26 FLO2ZT 27 36 F150A BB 26 PPS 7Z07901 57 FC FC APC fiber adapter 7Z08229 44 76 78 Female SM1 to SM1 Adapter 1G02260 44 FFC PH00203 210 Fiber adapter bracket for 4X beam expander SPG01649 178 Fiber adapter mounting bracket for 30 150 A BB 18 30 150 A LP1 18 7Z08211 44 Q OPHIR Spiricon Photon Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand OPHIR Photonics A Newport Corporation Brand OPHIR Photonics A Newport Corporation Brand 213 01 08 2013 Product P N Page Fiber adapter mounting bracket for 30A BB 18 30A N 18 7Z08211 44 Fiber adapter mounting bracket for 30A P 17 30 150 A SV 17 30 150 A HE 1 7 7Z08230 44 Fiber adapter mounting bracket for 3A IS 3A IS IRG 7Z08213 44 Fiber adapter mounting bracket for 50 150 A BB 26 50 150 A BB 26 PPS F150A BB 26 7708210 44 F150A BB 26 PPS Fiber adapter mounting bracket for FL250A BB 35 FL2
176. YAG 16 Mac Beam Powar va Beam Size Max Beam Power in atis lee Beam Width ii rma Model Beam Reduction Beam Sizes Wavelength Type of Attenuator Camera VY LPK YAG 2 5 FW LPK YAG 2 5 USB 1X 0l 25mm 1064nm 1 beam splitter assorted attenuators Si CCD N LPK YAG 7 FW LPK YAG 7 USB 3X 10 7 0mm 1064nm 1 beam splitter assorted attenuators Si CCD EN LPK YAG 16 FW LPK YAG 16 USB MOX ORCA 1064nm 1 beam splitter assorted attenuators Si CCD av PK YAG 16 18200 10X 3 0 16mm 1064nm 1 beam splitter assorted attenuators Si CCD amp i i 40 Ordering Information D Item Description P N n LPK YAG 2 5 USB BeamGage software SP620U camera LBS 100 YAG beam splitter attenuator base plate miscellaneous hardware SP90168 Suitable for beams 0 1 to 2 5mm S LPK YAG 7 USB BeamGage software SP620U camera LBS 100 YAG beam splitter attenuator 3X telescope base plate SP90169 oe miscellaneous hardware Suitable for beams 1 0 to 7mm LPK YAG 16 USB BeamGage software SP620U camera LBS 100 YAG beam splitter attenuator 10X telescope base plate SP90170 MM miscellaneous hardware Suitable for beams 3 0 to 16mm LPK YAG 16 18200 BeamGage software Gige 18200 camera bundled with BeamGage Enterprise LBS 100 YAG beam splitter SP90328 attenuator 10X telescope base plate miscellaneous hardware Suitable for beams 3 0 to 16mm Maximum beam size assumes zero diffraction from the wings of the beam Beams of up to 1 5X the maximum si
177. Z08212 Photodiode Sensors PD300R series and FPS 1 1G02259 7208227 7208226 7208229 1G01236 AEA ARG 7208213 7Z08227 7208226 7208229 1G01236 PD300 IRG not needed 7208216 7Z08222 General Accessories SH to BNC Adapter Allows connection of sensor to voltage measuring device for measurement of raw voltage output Z11010 IR Phosphor Card Glass slide 75x25mm with phosphor coating 25x50mm that visualizes spectral region 810 860nm 900 1100nm and 1500 1600nm Stands up to 1kW cm Oo cine Self actuating does not need charging from light source Female SM1 to SM1 Adapter For mounting PD300R and FPS 1 to SM1 optical components and systems 1G02260 Note a The fiber mounting bracket for these sensors is a triple adapter for mounting up to three different fibers looking at same spot and 7F01235A SC fiber adapter ST fiber adapter FC fiber adapter SMA fiber adapter 8 1 4 36 UNS 2A LS S SSS M20x1 i M8x0 75 M20x1 25 FC CONNE SC_F O CONNECTOR ST _F O CONNECTOR SM1 to M20 Adapter Mounting Bracket for PD300R Series 30A with F O input FL250A with F O input and FPS 1 P N 1G02259 53 Allows PD300R models to be used F O ADAPTER 26 F O ADAPTER a SI MOUNTING BRACKE
178. _ Configuration Screen Fian 10 0 Sensor Settings ibgd Press scroll down Pus Length 2 0us Diffuser MA key to select the Thranheid k n one s to adjust Context Sensitive Help Zero instrument electronics Shey Settings YEE Line Frequency SObz Jardin 12 26 mare it ood lake Scroll down to next parameter TE eee f i L y T Press to apply Offset kl Battery Status Fol D F Sh TASS Indicator Cairn teu Jani SS010 Sensor cimri 130 me ica information Mir ec Dees 2O012 Meter information Eat Exit to measurement screens Enter and update selected parameter Power Meter High legibility TFT 320 x 240 pixel graphics LCD Large 16mm digits High resolution analog needle also can be chosen Features Power single shot energy energy and frequency of high rep rate lasers position and size Outputs 1V Full Scale analog output Screen Refresh 15 times sec Case Molded high impact plastic with optimized angle kickstand Rubberized sides for easy grip and protection against damage Size Folds to a compact 213mm Lx 113mm W x 40mm H Battery changer also functions as an AC adapter Sensor Features PD300 sensors Submicrojoule and multikilohertz capability with pulsed energy sensors Rechargeable Li ion batteries with typically 8 hours between charges The charger can be ordered from your local distributor The Works with Thermopile BeamTrack Pyroelectric and Photodiode sensors Automatic
179. a Ooo OA 15 tO TOkHz Linearity with Energy for gt 10 of full scale 1 5 15 1 5 Damage Threshold J cm 0 1 0 1 0 1 Maximum Average Power mW 50 at 800nm 0 5 0 5 Maximum Average Power Density W cm 50 5 5 Maximum Energy vs Wavelength Wavelength Maximum Energy Wavelength Maximum Energy Wavelength Maximum Energy lt 300NM 15uJ lt 300nm 150nJ 800 900nm 20nJ 350 550nm 8uJ 350 550nm 75nJ 1000 1300nm amp nJ gt 800nm 5 gt 800nm 50nJ 1300 1400nm 7nJ 1480 1560nm 6nJ gt 1650nm 20nJ Fiber Adapters Available see page 76 ST FC SMA SC ST FC SMA SC ST FC SMA SC Weight kg O25 0 25 0 25 Version Part number Standard Sensor 7Z02944 7Z02945 7Z02946 Previous Model Part Number 7Z02823 7Z02824 7Z02827 Note a This is basic calibration accuracy In certain lt 250nm add 3 lt 250nm add 2 lt 900nm add 2 wavelength regions calibration there is additional erroras gt 950nm add 2 gt 950nm add 2 gt 1700nm add 2 tabulated here Note b With the user threshold setting set to minimum For other settings the spec is for gt 10 of full scale or greater than twice the user threshold whichever is greater The user threshold is available with Nova Il Vega StarLite or Juno For other meters the threshold is set to minimum and the linearity spec is gt 10 of full scale The PD C series will only operate with Nova or Orion meters with an additional adapter Ophir P N 7Z08272 see page 77 The adapter can introduce up to 1
180. acer 60X 60X Microscope objective SP90292 40X 40X Microscope objective SP90293 20X 20X Microscope objective SP90294 10x 10X Microscope objective SP90295 Y OPHIR Y Spiricon Photonics For latest updates please visit our website www ophiropt com photonics oy eee NES 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport A Newport Corporation Brand rporation Brand 3 5 2 EERIE 184 01 08 2013 3 5 2 Slit Based NanoScan Near Field Profiler Measuring the near field of sources such as laser diodes VCSELs optical fiber and or waveguides can be a difficult task Accurate measurement of such small sources to the micron level requires high precision in the optical and mechanical design To simplify this task and to fill this requirement Photon offers several models of Near Field Profilers NFPs covering a wide range of wavelengths and power levels Another important application of these instruments is to extend the focused laser spot size measurement range of the NanoScan profiler By expanding the size of a focused spot it is possible to reduce the power density and make possible the measurement of beams that are too powerful to be measured without attenuation as well as those that are too small to be accurately measured with the standard scanhead The NanoScan NFPs are easy to use turnkey systems that can be used either as a stand alone instrument or integrated into manufacturing inspecti
181. act wider dynamic range have higher repetition rates and measure longer pulses Through constant development Ophir again brings you the best performance in the market Heat sink disc t t Electrical leads RP Sensors The exclusive Ophir RP type heads represent a unique way of accurately measuring the energy of high average power and large duty cycle pulsed lasers while at the same time measuring average power and temporal pulse shape Principle of Operation RP heads incorporate an innovation patented that allows measurement of the energy of high energy repetitively pulsed lasers which is of advantages over pyroelectric measurement in certain cases higher average powers than a pyroelectric and high duty cycles up to 70 which are typical of switched diode lasers The basic approach is to incorporate two sensors in one measurement head The RP measurement head has a standard thermopile type detector enabling it to measure average laser power to a high degree of BNC connector to accuracy generally 3 In addition it contains a fast photodiode detector fast oscilloscope for Anpa Paez which measures the energy of the laser pulses in real time The photodiode detector is mounted so that a fraction of the radiation falling on the thermopile absorber 4 to 15 depending on head type is scattered from the absorber A fraction of that falls on the photodiode see illustration below there is also x a larger fast photodiod
182. adband gaai Spectral Range um 0 19 20 0 19 20 Aperture mm p 26mm p 26mm Power Mode Power Range 40mW 150W 50mW 150W Maximum Intermittent Power 150W for 1 5min 100W for 2 2min 50W continuous NA Power Scales 150W 50W 5W 150W 30W 3W Power Noise Level 2mW 8mW Maximum Average Power Density kW cm 12 at 150W 17 at 50W 12 at 150W 17 at 50W Response Time with Display 0 95 typ s 1 5 1 5 Power Accuracy 3 3 Linearity with Power 1 5 1 Energy Mode Energy Range 20mJ 100J 20mJ 100 Energy Scales 100J 30J 3 300m 100J 30 3J 300m4J Minimum Energy mJ 20 20 Maximum Energy Density J cm lt 100ns 0 3 0 3 0 5ms 5 5 2MsS 10 10 10ms 30 30 Beam Tracking Mode Position Beam Position Accuracy mm 0 1 0 1 Beam Position Resolution mm 2 5 of beam size 2 5 of beam size Min Power for Position Measurement 100mW 100mW Size Size Accuracy mm 5 for centered beam 5 for centered beam Size Range mm 40 beam diameter 3 20 3 20 Min Power Density for Size Measurement 1 W cm 1 W cm Cooling convection fan Fiber Adapter Available see page 44 ST FC SMA SC ST FC SMA SC Weight Kg 0 4 0 45 Version Part number Standard Sensor 7Z07900 7Z07901 StarLink Sensor Direct USB link to PC p 42 787200 Notes a The BeamTrack features are supported by Nova ll Vega and StarLite meters Juno interface and StarLab application Notes b For powers up to 30W it is recommended to work with the fan off
183. additional measurement error The user threshold feature allows adjustment of the internal threshold up to 25 of full scale if desired to avoid false triggering in noisy environments For highest accuracy it is recommended to zero the sensor against the meter the first time it is used with a particular meter For further information see the FAQs on our Website Note c Additional Error with Frequency of 1 on ly for energies up to 2uJ For higher energies 1 up to 10kHz 4 at 20kHz Note d Additional Error with Frequency of 1 only for energies up to 20nJ For higher energies 2 up to 10kKHz 5 at 20kHz PD10 C PD10 pJ C PD10 IR pJ C 5 22 Active Area 62 2x M2 5x6 deep ADJUSTABLE 90 139 ADJUSTABLE 90 139 OU OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand 1 3 2 Pyroelectric Energy Sensors 0 2uJ to 10mJ PE9 C Features o8mm and 12mm apertures PE10 C PE10BF C Previous Model Part Number PE 9 7Z02877 Repetition rates up to 25 000Hz a Highest sensitivity sensors Pulse widths up to 5ms C New compact PE C series W A N Model PE9 C PE10 C PE10BF C Use Most sensitive Sensitive High damage threshold Aperture m
184. ain Control used by Auto X and Auto setup Exposure Control used by Auto X and Auto setup Pixel Sampling Bits per pixel setting External Trigger Input Trigger Delay Strobe Output Strobe Delay External Trigger Probe Internal Trigger Probe These are features related to but not generally dependent upon the camera design Gamma Correction Gain Correction Bad Pixel Correction Lens Applied Option Pixel scale settings Magnification settings Frame buffer settings Ultracal Enable Auto X auto exposure control Perform an Auto Setup 8 amp 12 bits per pixel Select Format Measure S N ratio 01 08 2013 Features BeamMlc Laser Beam Analyzer Software VU OPHIR Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Ga Corporation Brand Y Spiricon OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand Trigger Capture and Synchronization Capture methods are features related to the application while Synchronization methods Methods System Requirements Ordering Information Item BeamMic USB2 Beam Analyzer Systems camera and software BM USB SP503 relate more to the abilities of the specific camera NOTE Frame capture rates are determined by many factors and are not guaranteed for any specific operating configuration Trigger modes a CW captures continuo
185. al ND UV o a a a a ee AAs 470 00 ii Aperture O20mmM Damage threshold 100W cm2 CW 10ns pulses no i distortion E a Lm Fi paheni rae Specialized Filters There are also specialized filters available to eliminate extraneous wavelengths when measuring very short or very long wavelengths where the CCD cameras are not sensitive and the desired signal can get swamped by extraneous light of other wavelengths These filters are as follows 3 4 1 PERMENO 1 The 355nm filter for monitoring the 3rd harmonic of YAG This filter transmits 355nm but blocks 532nm and 1064nm 2 The 1300nm filter transmits1300nm but blocks wavelengths shorter than 1100nm These filters are also on the same standard thread so they can be mixed with all the other components See ordering information pages for more details Y OPHIR Y ue Photonics For latest updates please visit our website www ophiropt com photonics Sy eee ES 01 08 2013 A Newport Corporation Brand A Newpor A Newport Corporation Brand orporation Brand Ordering Information Item _ Description Be PN ND1 stackable filter 4mm spacing screw on filter for camera with transmission of between 20 and 5 depending on spectral range SPZ08234 red housing Can be stacked and combined with other filters and beam splitters One filter is included with Spiricon cameras ND2 stackable filter 4mm spac
186. and then the noise level is 3 times lower It is also recommended to measure energy with the fan off Notes c Position accuracy for the central 10mm of the aperture as limited by beam position resolution Position can be tracked with 1mm accuracy over the entire aperture Accuracy is reduced by a factor of 3 at minimum power Notes d Assumes laser beam with Gaussian TEMoo distribution For other modes size measurement is relative Notes e Accuracy spec will be maintained for beams from 3 5 to 17mm not deviating from center more than 15 of beam diameter For beams below 8mm in size and powers above 75W error in size can reach 10 Interface Module on cable 50 150 A BB 26 PPS F150A BB 26 PPS aa cant 1 5M cable 0 5M cable to to sensor smart connector yd 2 Leet k ADJUSTABLE 140 ADJUSTABLE 95 140 DC power supply so Q OPHIR Phatinies For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand 1 2 3 Wyelawelas 58 01 08 2013 1 2 3 BeamTrack Power Position Size Sensors 150mW to 250W Features All the features of standard power sensors plus Accurate tracking of beam position to fractions of amm Monitoring of the laser beam size Model Use Absor
187. and with two beam splitters up to 400W The Beam Splitters will operate for wavelengths from 190nm to 2000nm The damage threshold of the beam splitters is gt 5J cm for 10ns pulses The beam splitters are mounted over the fixed or variable attenuators with a simple fastening ring and can be oriented in any direction with the beam coming from right left up down or front beam path One beam splitter mounted Two beam splitters mounted Fused silica reflectance at 45 degrees 12 TTT 6 HH P polarization 1000 2000 3000 The wedge angle of 10 degrees insures that only the reflection from the front surface will appear on the camera with no double images The user must insure that there are beam stops for the transmitted and reflected beams 3 4 3 CMEI Note that if possible the user should use an even number of beam splitters so as to cancel any possible polarization effects Average Percent reflectance per surface Wevelength nm 176 Y OPHIR Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand Ordering Information Item Description Aperture Pathlengthto CCD with P N 3 screw on ND filters 1st Wedge 45 degree wedged beam 15mm 60mm SPZ17015 Beam Splitter splitter to reduce intensities on image converter by 20X Aperture is 15mm 2nd
188. andard that has all of the BeamGage Standard features plus additional functionality Image Partitioning Partitioning allows the user to subdivide the camera image into separate regions called partitions and compute separate beam results within each partition When using partitioning special results items can be displayed that relate to delta values between the computed centroids or peaks of each partition Partitioning is useful to enable separate analysis of individual beams when multiple beams impinge on the camera simultaneously This feature is particularly useful when analyzing multiple fibers in a single bundle ew fe ac t Partitians Fa PosverEnengy Dien baa Liru Total Fer 50 Liet W Peak Fluence 150 1 3a2e 06 Weer i Man Fines 2 364e 03 Wie a Spatial ang tags al ee Unit Ceniki E EO SESS eetl um Centrodd EO Muell um Dow 140 EN um Dot mO e0 um Ddo 5O z siinid um Shown is an example of the results for partition P2 and its related display frame Observe that the selected partition is highlighted in RED The crosshair in each partition is user controlled The crosshair can be moved to a new position with the mouse or can be numerically positioned using the expanded controls that appear when a partition is created Automation Interface BeamGage Professional provides an automation interface via Net components to allow customers the ability to build custom applications that incorporate
189. ange amplification allows operation over many orders of magnitude in beam power From these profiles important spatial information such as beam width beam position beam quality and other characteristics are determined This technique can accommodate a wide variety of test conditions Because slit scanners measure beams at high powers with little or no attenuation they are ideal to profile beams used in material processing Carbon dioxide CO2 lasers are widely used in materials processing and have a 10 6 micron wavelength that cannot be profiled with most cameras Slit scanners therefore provide an convenient means of measuring high resolution CO2 lasers with powers up to and exceeding 1000 watts NanoScan Scanhead Aperture 2 Beam Characterization Detector Drum y 3 3 EMEIS Light Beam i P Light Beam Aperture 1 Beam Characterization Scanning Slits Q OPHIR Photon Photonics a Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics 01 08 2013 A Newport Corporation Brand 3 3 1 NanoScan 2 Scanning Slit Beam Profiler For High Accuracy Dimensional Measurementt NanoScan 2 now features direct USB2 connection to the PC and is available to measure CW and pulsed beams across the spectral range from UV to infrared up to 1800nm Coupled with the new NanoScan 2 software package that allows configuration of the user interface displays the Photon
190. ar 1 2 Juno USB interface Quasar or 4 legacy Bluetooth Ta Communication RS232 RS232 GPIB USB RS232 N A USB USB USB Bluetooth lt Method O Power Measurement U Power log period 5s to 24hr 12s to 600hr 12sto600hr NA 5s to 500hr 5s to 500hr 5s to 500hr 5s to 500hr Max points stored 300 5400 Nova ll5400 NA N A N A N A N A onboard Vega 27000 g Max points direct on PC unlimited unlimited unlimited N A unlimited unlimited unlimited unlimited U Analog output TIVES IVES 1V 2V 5V 10V IVES N A N A IVES N A Co z Energy Measurement O Max real time data gt 10Hz gt 30Hz RS232 gt 2000Hz USB NA 25 000Hz 10 000Hz 2000Hz 500Hz az logging to PC gt 1500Hz GPIB gt 30Hz RS232 Max onboard data logging gt 10Hz OOR A0002 N A N A N A N A N A mM rate N Data transfer rate of a 50 points s 500 points s 500 points s N A N A N A N A N A data file from instrument N to PC Max points stored 1000 54 000 Nova Il 60 000 N A N A N A N A N A onboard Vega 250 000 Trigger input and N A N A N A N A BNC trigger N A N A N A output input to enable measurement of missing pulses Can also be configured to give trigger output Timing time stamp for N A N A N A N A resolution 1us resolution resolution resolution each pulse 10us 50ms 10ms General Automation Interface no no yes N A yes yes yes no LabVIEW VIs yes yes yes N A yes yes yes no Maximum baud rate 19200 38400 38400 N A N A N A N A N A PC file format Text files soreadsheet compatibl
191. ard ISO DIN 11146 Results measured include Beam Width at various clip levels m Centroid Position m Peak Position m Ellipticity m 1D Gaussian Fit m Beam Divergence m Beam Separation m Pointing Stability RO Power optional Total Power optional m Peak in digitizer counts m Pulsed Laser Repetition Rate Both docked and undocked windows Result ROIZ Value Mean S Dev 13 5 Width Al um 1 63 328 B64612 0 7082 13 5 Width A2 urn 1 876317 875 622 0 9432 Dagma Al ur 1 649 062 843 700 1 354 Disigma A2 prm 42 054 B40 924 23751 Centroid Position Al pra 1 1111 0133 05522 Centroid Postion AX im 1 730 O275 1 2221 Peak Position Al urm 1 11 521 19 890 55014 Peak Position AJ ym I 4156 8732 6 9860 Peak Al ents 1 2812438 2510 585 4 0456 Peak A ents 1 2687898 2678320 5 5879 Ellipticity 1 0 506 0807 0 0025 Power 3 1 79 Fid 479 00273 Total Power mi 1 202 1203 0 0007 Example of the many measurements that can be made and the precision you can expect an E POr SS ipp ie E Er Hp bee oa m i ina Ei aa iim rE an 4 au ne an um Bt EN E EHE Wa prs na ne te BB ma a4 ifi EEL r EzE E OA a A i u E fi E u i Knowing pointing stability is a critical factor in laser performance Photon VU OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics
192. are BGS FWB GRAS20 DESKTOP BeamGage Standard software software license 1 1 8 format 1600x1200 1394b camera with 17 5mm C mount SP90202D recess Comes with 1394b and trigger cable PCI Express interface card and 3 ND filters Desktop model BGS FWB GRAS20 LAPTOP BeamGage Standard software software license 1 1 8 format 1600x1200 1394b camera with 17 5mm SP90202L C mount recess Comes with 1394b and trigger cable Laptop PCI Express interface power supply and 3 ND filters Laptop Model BGS FWB GRAS20 1550 DESKTOP BeamGage Standard software software license 1 1 8 format 1600x1200 Phosphor coated 1550nm SP90203D sensor 1394b camera with 17 5mm C mount recess Comes with 1394b and trigger cable PCI Express interface card and 3 ND filters Desktop model BGS FWB GRAS20 1550 LAPTOP BeamGage Standard software software license 1 1 8 format 1600x1200 Phosphor coated 1550nm SP90203L sensor 1394b camera with 17 5mm C mount recess Comes with 1394b and trigger cable PCI Express interface card and 3 ND filters Laptop Model BeamGage Professional USB2 Beam Profiler Systems camera and software BGP USB SP503 BeamGage Professional Edition software software license 1 2 format 640x480 pixel camera with 4 5mm SP90236 CCD recess Comes with USB cable and 3 ND filters BGP USB SP503 1550 BeamGage Professional Edition software software license 1 2 format 640x480 pixel camera with 4 5mm SP90237 CCD recess Phosphor coa
193. atellite windows on multiple monitors Continuous zoom scaling in both 2D and 3D Camera ROI support Manual and Auto aperturing to reduce background effects Pass Fail on all results items w multiple alarm options Results logging capabilities in a reloadable Industry standard data file format Configurable Report Generator that allows cut and paste of results images and settings Supports English German Japanese and Chinese Windows OS in both 32 and 64bit Multilingual GUI in English Japanese and Chinese per ISO 11145 11146 1 3 and 13694 Total power or energy Peak power energy density Min Fluence Peak and Centroid locations Beam width Second Moment D4s Knife Edge 90 10 Knife Edge User selectable level Percent of Peak User selectable a Percent of Total Energy User selectable Encircled power smallest slit 95 4 a Moving Slit User Selectable Beam diameter E E Average diameter based on x y widths Second Moment D4s liptical Results Elliptical orientation Ellipticity a Eccentricity Continuously zoomable and resizable displays in satellitable window Continuous Z axis display magnitude scaling Zoomable to subpixel resolution for origin and cursor placements Pixel boundaries delinated at higher zoom magnifications Adjustable Cursors that can track peak or centroid Adjustable manual apertures Viewable Auto aperture placemen
194. athmatica Math program and Excel compatable ASCIl csv results files Graphics in jg file format Legacy file compatability with LBA formats A user defined single file output that can contain settings beam displays beam profiles charts results etc in either pdf or xps file formats Printing Images reports results graphs charts statistics and setup information Option to print many frames in a single operation WYSIWYG images Pass Fail Set Maximum Minimum limits on all calculations and statistics Red Green font color indication on result items Multiple choices for indication of failed parameters including TTL pulse for external alarm Master pass fail which triggers alarm on any failure USB signal beep stop and log alarm options Logging Video Data Logging Formats HDF5 ASCIl csv Results in ASCIl csv Pictures 2D and 3D in jpg gif tiff bmp png file formats Charts in ASCll csv Cursor Data in ASCII csv Row Column summed in ASCIl csv Continuous Logging Time Interval Logging Frame Count Logging Periodic Sampling Pass Fail Sampling Burst Sampling after a user specified time interval sample a user specified number of frames Exporting Convert frame buffer data to third party format Export a user specified number of frames from the buffer Export Image Data ASCIl cvs Export Results ASCIl csv Export Picture jpg gif tiff bmp png file formats supported Export Cur
195. ber Type Spectral Range um Aperture mm Power Mode Power Range Power Scales Power Noise Level Maximum Average Power Density kW cm Response Time with Display 0 95 typ s Power Accuracy Linearity with Power Energy Mode Energy Range Energy Scales Minimum Energy mJ Maximum Energy Density J cm lt 100ns O0 5ms 2MS 10ms Beam Tracking Mode Position Beam Position Accuracy mm Beam Position Resolution mm Min Power for Position Measurement Size Size Accuracy mm Size Range mm 40 beam diameter Min Power Density for Size Measurement Cooling Fiber Adapter Available see page 44 Weight Kg Version Part number Standard Sensor StarLink Sensor Direct USB link to PC p 42 Notes a The BeamTrack features are supported by Nova Il Vega and StarLite meters Juno interface and StarLab application Notes b For powers up to 50W it is recommended to work with the fan off and then the noise level is 3 times lower It is also recommended to measure energy with the fan off Notes c Position accuracy for the central 20mm of the aperture as limited by beam position resolution Position can be tracked with 1mm accuracy over central 32mm of the aperture Accuracy is reduced by a factor of 3 at minimum power Interface Module on cable 77 et 1 5M cable 0 5M cable to to sensor smart connector vt FL250A BB 50 PPS FL250A BB 50 P
196. between repetition rate sensitivity and maximum pulse width If standard products are not suitable these parameters can be tailored to customer requirements PE10 S Q MOUNTING HOLES 2x 5 7 2x 3 2 Q OPHIR Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand WY N U VN gt ac 31 01 08 2013 1 3 7 1 Balawelss 01 2 PHIR 1 3 7 1 Standard OEM Pyroelectric Energy Sensors 0 1mJ to 10J PE25 S PE25BB S PE25 A DIF XXX YYY PE25BB S DIF Features Compact Low Profile Low Cost With built in electronics for complete self contained OEM solution with calibrated square pulse output The following specifications refer to standard OEM sensors and are to be understood as generic describing sensor families Ophir will be happy to help you with a specific solution for your particular application Model PE25 S PE25BB S PE25BB S DIF PE25 A DIF XXX YYY Features General purpose Spectrally flat High damage Built in amplifier Output of calibrated threshold square pulses Aperture mm 24 x 24 24 x 24 20 p 24 Absorber Type Metallic Broadband Broadband diffuser Metallic diffuser Spectral Range um 019 3 0 19 20 0 4 3 0 4 3 Surface Reflectivity approx 50 10 15 ips Calibration Accuracy 3 a a 3 Sensitivity approx at 1064nm 9V J into IMO 5 5V J into IMQ 2
197. calibrated for 10 6um as well To measure CO laser set to the 3000nm setting The additional error for measuring 10 6um is 5 Note f Add 3 to error for wavelengths gt 2um Note g For PE9 C with the Laserstar Pulsar USBI Quasar and Nova Orion with adapter only 2 of the 3 pulse width settings are available the 1us and 2us settings peel p21 PE9 C PE10 C PE10BF C 10 5 10 5 100 75 Q OPHIR 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand 1 3 2 Pyroelectric Energy Sensors 8uJ to 10J Features 24mm apertures Metallic coating for high rep rates PE25 C PE25BF C Energy Sensor with optional heat sink N m BF coating for highest damage threshold Rep rates up to 10kHz E Measure lasers with pulse ap widths up to 20ms 2 New compact PE C series N Model PE25 C PE25BF C ymm Use High rep rate High damage threshold Aperture mm p24 p24 Absorber Type metallic BF Spectral Range um 0l Cisse Surface Reflectivity approx 50 20 Calibration Accuracy 3 3 Max Pulse Width Setting 2uUs 30us 500us ims 5ms Ims 2ms 5ms 10ms 20ms Z 10J to 10J to 10J to 10J to 10J to 10J to 10J to ee 10 to 10J to NEGY cals 200W
198. charger also functions as an AC adapter Data Handling Data can be viewed on board or transmitted to PC On Board Non volatile storage of up to 54000 data points in up to 10 files Max data logging rate 4000 points s Transmitted to PC Data transmission rate of 500 points s RS232 baud rate of 38400 Sensor Features Works with Thermopile BeamTrack Pyroelectric and Photodiode sensors Automatic continuous background cancellation with PD300 sensors Submicrojoule and multikilohertz capability with pulsed energy sensors Program Features Preferred startup configuration can be set by user User can recalibrate power energy response time and zero offset Notes a The above refers to the rate of logging every single point in turbo mode Above that rate the instrument will sample points but not log every single point Ordering Information Item Description Ophir P N Nova Il Nova Il universal power meter for thermal pyroelectric and photodiode sensors 7Z01550 Carrying Case Carrying case 38x30x11 cm For power meter and up to three sensors 1J02079 Nova Il USB Cable USB to mini DIN cable 1 unit supplied with Nova II 7E01205 Nova II RS232 Cable D9 to mini DIN cable 1 unit supplied with Nova Il 7E01206 Battery Pack Replacement battery pack for the Nova II 7E14007 lt Q OPHIR 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 2 1
199. cm lt 100ns 0 3 0 3 0 05 0 3 0 05 1us 0 5 0 5 0 3 1 0 3 0 5ms 5 5 20 5 15 2MS 10 10 50 10 40 10ms 30 30 150 30 200 Cooling fan fan fan fan fan Fiber Adapters Available see page 44 ST FC SMA SC STEC OMA SG ST FC SMA SC NA NA Weight kg 0 8 0 9 0 9 2 7 2 7 Version Part number Standard Sensor 7Z02739 7Z02734 7Z02735 7Z02648 7Z02667S BeamTrack Sensor Beam Position amp 7Z07902 Size p 58 Notes a For lower powers up to 50W it is recommended to work with the fan off and then the noise level is 3 times lower It is also recommended to measure energy with the fan off Notes b LP1 sensors have relatively large spectral variation in absorption and have a calibrated spectral curve at all wavelengths in their spectral range to the above specified accuracy Nova and Orion meters do not support this feature and when used with those meters accuracy will be 3 for 532nm 808nm 1064nm and 2100nm and 6 for other wavelengths in the spectral range 400 1100nm FL500A FLSOOA LP1 FL250A BB 50 FL400A BB 50 FL400A LP 50 120 i l 120 T j 36 1 l ADJUSTABLE H 7 Jas 122 168 hat 37 ADJUSTABLE 107 153 TA Q OPHIR a Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand 1 1 2 6 High Power Water Cooled Thermal Sensors and Power Pucks 1W to 300W Features High powers L250W L300W LP
200. consistent results for M values for lasers that are not exactly like those for which the ISO standard was written such as fiber lasers lensed diode lasers and VCSELs 3 6 2 EERIE EIV The NanoScan Difference With the NanoScan equipped NanoModeScan all scan heads can measure pulsed beams with repetition frequencies down to 10kHz Measuring pulsed beams in discussed in the application note Measuring Pulsed Beams with a Slit Based Profiler The silicon and germanium detectors will measure less than a milliwatt of power The pyroelectric detector equipped NanoScan head can analyze higher power lasers at all wavelengths The increased dynamic range of the NanoScan enhances the signal to noise ratio of the system and allows a much broader range of laser powers to be analyzed with one instrument setup on Q OPHIR Photon 01 08 2013 seule For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporatio A Newport Corporation Brand Real Time Divergence Measurement By monitoring the divergence angle 9 it is possible to make a measurement that will be directly proportional to M This enables the adjustment of the laser performance in real time at the NanoScan s rapid update rate up to 20HZz To use this feature the scan head is moved to a position one geometric focal length from the test lens Divergence is the beam diameter divided by the focal length and the meas
201. continuous background cancellation with Ordering Information Item Description Ophir P N StarLite StarLite universal power meter for Thermal BeamTrack Pyroelectric and Photodiode sensors 7201565 Carrying Case Carrying case 38x30x11 cm For power meter and up to 3 sensors 1J02079 USB Cable for StarLite USB A to MICRO B cable for field upgrade support 1 unit supplied with StarLite 7E01279 7E14008 Battery Pack for StarLite Replacement battery pack for the StarLite Q OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics 2 1 6 ACCESSORIES RS232 Module for Nova Plug in module allows transfer of power and energy data to PC and remote control of power meters from PC Includes manual and Starcom application program refer to page 107 IEEE488 GPIB for Laserstar Option available with Laserstar power meter allowing Laserstar to operate with GPIB protocol The option comes with Starcom software and also LabVIEW VIs to build LabVIEW applications Carrying Cases Carrying case for Vega Nova Il StarLite or Nova power meters and up to 3 sensors 1 6 BRON elaAleltelas Ordering Information Item Description Ophir P N Nova RS232 Assembly RS232 adapter with standard 2 meter cable including software 78105 Nova RS232 Assembly RS232 adapter with 5 meter cable including software 781052 Nova RS232 Assembl
202. creens Digital Power Screen basei 3 e ERE Active sensor CW industrial medical and scientific lasers 3 15 1 0s for multisensor power meter pW to multi kW with appropriate sensors s Ws SaN V m Can average over selected period Useful for unstable lasers bi a se hl rb Meal oro lr Poni m Fast response bar graph Change Zoom Subtract Change Access t b h offset further fucti Laser Tuning Screen or Power Log Screen not shown A a a a a meer ingen a Maximizing laser power m User selected time period and zoom NOH m Option of audio tune tone for maximizing laser power B a7o0 son setur max esc Previous sreen Change Set settings maximum reading O OPHIR Zo For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand orporatio PESO Ve 0 enera A 0593 NG mie ania max 3045 2ml Present energy range laser ranse menu Energy Measurement Screen Laser m Pyroelectric and thermal Frequency sensors single pulse Change to power m Pyroelectric frequency Select average Access further measurement periodornone Trigger Change laser Change functions indication wavelengh range Energy Log Screen Store every pulse m Pulsed energy sensors m Thermal sensors successive single pulses m Continuous scroll m Energy statistics screen Enter statistics Temporary pause Reset Zoom reading statistics of showing p
203. cs A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand 3 8 4 High Power ModeCheck A New Method to Assure the Performance of High Power CO2 Lasers Beam Profiler for collimated 50W 500KW 10 6um wavelength beam width up to 30mm Laser Beam In Quality Cutting Marking Drilling amp Ablating Require More Than Consistent Laser Power Instantaneously see and measure the beam reduce set up time between jobs Real time mode burns eliminate hazardous acrylic vapors Optimize laser efficiency reduce cost per part Predict laser preventative maintenance increase manufacturing efficiency ModeCheck is designed for the industrial parts manufacturer to reduce the time it takes to change over between different jobs The user can quickly place the ModeCheck in front of the laser and see and measure in real time the laser beam profile to confirm optimal laser performance In addition and when used periodically the user can compare measurement changes from the same set up and make necessary laser adjustments keeping the laser output constant for the same job from day to day Over time the user will be able to see and measure laser degradation to predict and advance schedule down time needed for periodic maintenance Pass Through Beam Out ModeCheck eliminates operator exposure to acrylic mode burn hazards while improving product quality and manufacturing efficiency Measurements In ad
204. cs For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 1 3 4 RP Sensors 200mW to 1500W Features Very long pulse repetitive lasers m Energy measurement at high average powers Pulse rates to 15kHz Pulse widths to 200ms Temporal pulse shape measurement into scope FL250A RP L1500W LP1 RP Model FL250A RP Use Long pulse lasers Absorber Type Broadband Spectral Range for Power um 0 19 6 Spectral Range for Energy um 0 4 1 1 Aperture mm o50mm Power Mode Power Range 200mW to 250W Power Scales 250W 30W Power Noise Level mW 10 Maximum Average Power Density kW cm 8 Response Time with Display 0 95 typ s 25 3 Power Accuracy Linearity with Power Minimum Average Power Energy Mode Energy Range Energy Scales 1 200mW 100J to 1mJ 100J to 30mJ Energy Accuracy for energies gt 30 of full scale 5 Minimum Energy Maximum Pulse Width ms Stabilization Time s Maximum Energy Density and Rep Rate vs Pulse Width Pulse Shape Photodiode Response lime Peak Voltage into 50Q 1mJ in repetitive mode 50mJ in single shot mode 200 6 Pulse Width J cm pps lt 10us 0 3 15000 O0 5ms 5 1400 5ms 20 150 100ms 400 7 Tus 0 8V for 1kW peak power at 1064nm System Specifications with USB PC Interface Frequency Measurement Accuracy Statistics Displayed Maximum Data Acquisition Rate Cooling Weight kg Version Part n
205. ction to Camera Based Profilers 117 3 2 1 BeamGage 118 A ae lal BeamGage Standard 118 oD PIF BeamGage Professional 126 D PAE BeamGage Enterprise 126 3 2 1 4 Software Comparision Chart Izy 5 3 2 2 BeamMic Basic Laser Beam Analyser System 135 U 3 2 3 Cameras 140 Z 3 2 3 1 190 1100nm USB Silicon CCD Cameras 140 F 190 1100nm Firewire Silicon CCD Cameras 142 EE 32 3 2 190 1100nm Gig E Silicon CCD Cameras 143 323A 1440 1605nm Phosphor Coated CCD Cameras For NIR Response 144 O oer 900 1700nm InGaAs NIR Cameras 147 N 3 2 4 13 355nm and 1 06 3000um Pyroelectric Array Camera 148 3 24 1 YAG Focal Spot Analyzer 155 33 Introduction to Scanning Slit Profilers 157 EA NanoScan 158 gl 3 4 Accessories for Beam Profiling 168 aa 3 4 1 Neutral Density Attenuators Filters 168 5 3 4 2 Beam Splitter Neutral Density Filters Combo 172 G 3 4 3 Beam Splitter 175 lt 3 4 4 Beam Expanders Microscope Objectives o 177 345 Beam Reducers es 179 346 CCTV lens for front imaging through glass or reflected surface 180 ga 347 Imaging UV lasers 181 as 3 5 Near Field Profilers 183 cred Camera Based Near Field Profiler 183 O 3 9 2 Slit Based NanoScan Near Field Profiler 184 A 3 6 What is M er 3 6 1 M 200s Camera Based Beam Propagation Analyzer M 187 3 6 1 1 Specifications for the M 200s 189 BG lie Model 1780 190 362 Slit Based Beam Propagation Analyzer M 192 3 7 Integrated Laser Performance Measurements 195 3 7 1 Beam Cube 195 3
206. cy of hold time is 20 Maximum hold time limited to 50 of duty cycle At end of hold time voltage drops to below 0 2V PE25 S PE25BB S PE25 A DIF XXX YYY __ Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand 1 3 7 1 Standard OEM Pyroelectric Energy Sensors 1mJ to 10J Features Large apertures Compact Low Profile Low Cost The following specifications refer to standard OEM sensors and are to be understood as generic describing sensor families Ophir will be happy to help you with a specific solution for your particular application PE50 S PESOBB S 1 3 7 1 Biases Model PE50 S PESOBB S Features Large aperture Large aperture spectrally flat Aperture mm o 46 o 46 Absorber Type Metallic Broadband Spectral Range um 0 19 3 0 19 20 Surface Reflectivity approx 50 5 Calibration Accuracy 3 3 Sensitivity approx at 1064nm 2 5V J into IMQ 1 8V J into IMQ Max Pulse Width 800us 2ms Maximum Pulse Rate pps 10 10 Maximum Energy 10J 10J Minimum Energy ImJ 10mJ Noise Equivalent Energy approx 20uJ 0 5mJ Output BNC BNC Damage Threshold for 10ns pulses J cm lt 100nm 0 1 0 3 Tus 0 2 0 3 300us 2 1 Maximum Average Power W 20 15 Maximum Average Power Density W cm 10 10 Dimensions 75 x 14mm 75 x 14mm Part Number Consult Ophir representative Consult Ophir representative Notes a At calibrated wav
207. d YAG laser both with cavity misalignment The camera is also useful in product engineering of CO and other infrared lasers The Pyrocam III is an integral part of the assembly lines of many CO laser manufacturers Integrators of systems are using the Pyrocam sensor to make sure that optical systems are aligned and operating properly CO laser with cavity misalignment Nd YAG laser with cavity misalignment There are many medical applications of the Pyrocam Ill such as the analysis of excimer lasers used for eye surgery In many cases these lasers need alignment to ensure that the eye surgery is performed as expected Other medical IR lasers perform dermatology for which the uniformity of the beam profile must be assured Fiber optic communications at 1 3um and 1 55um make significant use of the Pyrocam III for analyzing the beams being emitted as well as analyzing properties of the beams before launching them into fibers The greater stability of the Pyrocam III make it a good choice over other cameras operating at telecommunication wavelengths 3 2 4 ERRIMEN CO laser with cavity misalignment Nd YAG laser with cavity misalignment Y OPHIR Y ea Photonics For latest updates please visit our website www ophiropt com photonics A 01 08 2013 A Newport Corporation Brand A Newpor A Newport Corporation Brand orporation Bral The Pyrocam Ill is becoming an essential tool in the maintenance of industrial inf
208. d for UV wavelengths 250 400nm PH00097 UV200 200mm focal length lens PH00098 UV250 250mm focal length lens PH00099 UV350 350mm focal length lens PH00100 UV500 500mm focal length lens PH00101 UV750 750mm focal length lens PH00102 UV1000 1000mm focal length lens PH00103 MS VIS Lens Kit MS VIS kit Visible VIS lenses are all BK 7 plano convex and coated for visible wavelengths 450 650nm PH00104 VIS200 200mm focal length lens PH00105 VIS250 250mm focal length lens PH00106 VIS400 400mm focal length lens PH00107 VIS500 500mm focal length lens PH00108 VIS750 750mm focal length lens PH00109 VIS1000 1000mm focal length lens PH00110 MS NIR Lens Kit MS NIR kit NIR lenses are all BK 7 Plano convex and coated for NIR wavelengths 700 1100nm PH00111 NIR200 200mm focal length lens PHO0112 NIR250 250mm focal length lens PH00113 NIR400 400mm focal length lens PH00114 NIR500 500mm focal length lens PH00115 NIR750 750mm focal length lens PH00116 NIR1000 1000mm focal length lens PH00117 Extension and Focusing Tubes CM EXT100 100mm long C Mount extension tube for mounting lenses outside ModeScan 1780 Box PH00119 CM EXT50 50mm long C Mount extension tube for mounting lenses outside ModeScan 1780 Box PH00120 CM EXT40 40mm long C Mount extension tube for mounting lenses outside ModeScan 1780 Box PH00121 CM EXT25 25mm long C Mount extension tube for mounting lenses outside ModeScan 1780 Box PHOO1 22 CM EXT10 10mm long C Mount extension tube for mounting lenses outside M
209. d for installation to desktop PC s Card has both 1394a and 1394b SP90164 Desktop Card compatible ports Compatible with all LBA and BeamGage FireWire systems 1394b FireWire Cable 1394b FireWire cable 4 5 meter length SP90166 1394a b Adapter Cable 1394a 6 to 1394b 9 adaptor cable 4 5 meter length SP90207 1394b FireWire Power Supply External Wall cube power supply for 1394b CardBus and PCI Express 34 Laptop Adapters SP90167 USB A B Cable USB Cable with A to B connectors 5 meter length SP90204 USB A mini B Cable USB Cable with A to mini B connectors 5 meter length SP90205 USB Pass Fail Cable Output Pass Fail signals when BeamGage is in out mode SP90060 Optical Synch for Pulsed Lasers Optical Trigger for FX and SP Cameras Optical trigger assembly which can be mounted on camera or separately to sense laser pulses and SPZ17005 synchronize FX and SP cameras with pulses Comes with a BNC cable Stand for mounting sold separately 3 2 1 4 CEMAES 134 Y OPHIR Y Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand Newport Corporation Brand BeamMic Basic Laser Beam Analyzer System High speed false color beam intensity profile displays in both 2D and 3D Operates in Windows 7 32 64 VISTA 32 64 and XP 32 Professional Numerical beam profile analysis employs pate
210. d temperature variations Notes c For position within inner 30 of aperture Notes d Assumes laser beam with Gaussian TEMo distribution For other modes size measurement is relative Notes e For P type and shorter wavelengths derate maximum energy density as follows Wavelength Derate to value 1064nm not derated 532nm not derated 355nm 40 of stated value 266nm 10 of stated value 193nm 10 of stated value Interface Module on cable 3A QUAD 3A P QUAD 10A PPS 1 5M cable 0 5M cable to i m r n ee to sensor smart connector oe j a sa Ps QUAD 012 n ares 3A QUAD 20mm ise a S AF REMOVABLE PART M20x1 x4 deep Y 97 143 ADJUSTABLE Surf ATT 11 5 1 16 ADJUSTABLE 92 127 O w Photonics A Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics 1 2 2 BeamTrack Power Position Size Sensors 50 150 A BB 26 PPS F150A BB 26 PPS 40mW to 150W Features All the features of standard power sensors plus Accurate tracking of beam position Ta to fractions of amm O Monitoring of the laser beam size N U UY Model 50 150 A BB 26 PPS F150A BB 26 PPS N Use General purpose General purpose Absorber Type Broadband Bro
211. d with rotation mount 12 5mm entrance aperture and matched pair of 25micron wide slits USB USB NS PYRO 9 5 STD NanoScan Pyroelectric Detector 9mm aperture 5micron slits High resolution head featuring pyroelectric PH00396 detector 63 5mm diameter head with rotation mount 9mm entrance aperture and matched pair of 5um wide slits Use for wavelengths from 190nm to gt 20um This model does not include a cooling fan USB USB NS PYRO 9 5 PRO Software includes automation feature PH00025 NanoScan Pyroelectric Detector 9mm aperture 5micron slits High resolution head featuring pyroelectric detector 63 5mm diameter head with rotation mount 9mm entrance aperture and matched pair of 5um wide slits Use for wavelengths from 190nm to gt 20um This model does not include a cooling fan USB USB NS PYRO 9 25 STD NanoScan Pyroelectric Detector 9mm aperture 25micron slits High resolution head featuring PH00400 pyroelectric detector 63 5mm diameter head with rotation mount 9mm entrance aperture and matched pair of 25um wide slits Use for wavelengths from 190nm to gt 20um This model does not VY include a cooling fan DH USB NS PYRO 9 25 PRO Software includes automation feature PH00228 NanoScan Pyroelectric Detector 9mm aperture 25micron slits High resolution head featuring O pyroelectric detector 63 5mm diameter head with rotation mount 9mm entrance aperture and matched pair of 25um wide slits Use fo
212. de 7Z02505 Optional Accessories and P N ND1 nom x10 attenuator 7Z08200 ND2 nom x50 attenuator Z08201 Fiber adapters SMA 1GO1236 e 7208229 SE 7Z08227 ST 7208226 SM1 to M20 adapter 1 necessary for above adapters and or attenuators 1G02259 FPS 1 Spectral Response Without Filters 0 5 7 M Pee ma Battery On Off 04 ff p P 9 2 BNC Connector a D LO 4 035 40 SM1 i Alternate Pole g 2 Mounting Thread po 5 So R 9 5 j a oe B a2 Battery housing _ 7 J r r Pare a n Detector Surface pia 200 400 500 600 700 B00 900 1000 1100 1 4 20 REF 1 4 20 BSWx6 deep Mounting Thread Wavelengih nm Q OPHIR 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 1 3 7 OEM Solutions Introduction Many laser systems manufacturers need to have a measuring capability built into their systems Ophir is the world s leading supplier of OEM laser power energy measurement instrumentation which can be built into host systems such as medical industrial etc With extensive experience accumulated in the field Ophir offers the largest variety of OEM products and is therefore best able to satisfy customer requirements Many configurations possible An OEM solution is usually needed to monitor laser performance i
213. de Sensors 10pW to 300mW Features Spectral range including UV and IR Very large dynamic range Swivel mount for hard to measure places Comes with filter in filter out options Fiber optic adapters available PD300 with filter off PD300 with filter installed PD300 IRG with no fiber input PD300 IRG with fiber input 1 1 1 1 Bfetatseras Model PD300 UV PD300 IR PD300 IRG Use Lowest powers from 200 1100nm Low powers from 700 1800nm_ Telecom wavelength fiber and free space measurements Detector Type silicon germanium InGaAs Aperture 10x10mm osmm 5mm for free space beams Filter mode Filter out Filter in Filter out Filter in Filter out Filter in Spectral Range nm 200 1100 220 1100 700 1800 700 1800 800 1700 950 1700 Power Range 3mW to 200W 300mW to 30mW to 5nW 300mW to 800uW to 10pW 150mW to 20uW 2uW 200W Power Scales 3mW to 3nW and dBm 300mW to 30MW to 30nW 300mW to 800 uW to 800pW 300mW to 3mW 300uW and dBm and dBm 30mW and dBm and dBm and dBm Resolution nW 0 001 100 0 01 NA 0 0001 1 Maximum Power vs Wavelength nm mW mW nm mW mW nm mW mW 250 350 3 300 800 12 120 lt 1000 08 100 400 3 300 1000 30 300 1100 0 8 30 1300 600 5 300 1400 30 250 1200 0 8 50 800 950 25 150 1500 25 80 gt 1300 08 150 1064 3 30 1600 30 100 1800 30 300 Accuracy including errors due to temp variations error vs Wavelength nm 6 200 270 10 220 400 5 700 900 7 700 900 3 1000 1650 6 1000 1650 3 270 950 5 400 950 4 900 1700 6 900 1
214. distances from a lens coupled with the known characteristics of the focusing lens M Measurement Solutions Ophir Spiricon and Photon have a number of solutions for the measurement of M ranging from simple manual processes to fully auto mated dedicated instruments depending on the frequency of the need to measure M of lasers and laser systems We have a system that will meet most needs whether for research and development of new laser systems manufacturing quality assurance or maintenance and service of existing systems 3 6 EERME Foeusing Lane uae Y OPHIR Spiricon Photon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics OPHIR Photonics A Newport Corporation Brand En Corporation Brand A Newport A Newport Corporation Brand Brand A Newport Corporation Brand 3 6 1 Camera Based Beam Propagation Analyzer M M2 200s Automatically measure your beam quality in under 2 minutes Tune your laser for best operation a SO compliant a Specifically developed for continuous usage Unequaled accuracy using patented Ultracal Calibration Automatic attenuation adjustment Pulsed and CW for most beam diameters and powers a Compact and portable Not all commercial M measuring instruments conform to the ISO 11146 method of employing a fixed position lens and moving detector Instead some manufacturers use a fixed position detector
215. dition to both 2D and 3D graphical image display and save the following measurements are made from each image Beam Widths and Diameters Beam Position Stability Power Density Peak Beam Centroid Location Elliptical Analysis with Major Axis Orientation It s just this easy 1 Remove Focusing optic Locate the beam center with pointing beam or similar device Place ModeCheck in beam center s Turn on Laser Instantly see measure and electronically store the beam characteristics ui BW N Optional Accessories One must manage the pass through laser beam by collecting the beam using either a power meter or beam dump We recommend using a power meter as the additional measurement information will assist in managing laser optimization Note that any beam dump or power meter large enough to handle 5kW will require water cooling There are holes on the bottom of ModeCheck for mounting the Power Meter Head or Beam Dump 3 8 4 PERMES A ruggedized storage carrying case is highly recommended for safe and efficient handling p i am EE E The ModeCheck Lens Adapter MLA is an option that will enable a ModeCheck to recollimate a focused CO2 laser beam The advantage of using this adapter is that the focusing head of the machine does not have to ModeCheck makes instantaneous beam measurements along be removed which is the normal case for a ModeCheck without this adapter with graphically displaying both the
216. e NanoScan aperture all with sub micron precision The optimal pro software includes ActiveX automation for users who want to integrate the NanoScan into OEM systems or write their own user interface screens M Wizard M squared M software Wizard is an interactive program for determining the times diffraction limit factor M by the Rayleigh Method The M Wizard prompts and guides the user through a series of manual measurements and data entries required for calculating M The Optional Rayleigh Range Translation Test Fixture RAL FXT provides convenient translation of a NanoScan scanhead assembly and a digital readout of its relative position along the Z axis Used with a user provided focusing lens and the M Wizard in the NanoScan Analysis Software this fixture offers a quick and easy method to determine the times diffraction propagation factor M of a laser The optional Translation Test Fixture makes manual M2 measurements accurate and repeatable The RAL FXT features a base plate sliding carriage and digital micrometer The base plate 5 4X10 2x0 38in provides a series of 14 20 threaded mounting holes at 2in centers to facilitate convenient fixturing of the assembly with respect to the focusing lens The sliding carriage accommodates the combination of the 0 125 in dowel pin and the 14 20 mounting hole found on any Photon scan head s rotation mount and enables smooth movement of the scan head assembly over a 6 in
217. e smart sensor O18mm 0 19 20um 60mW 100W A48x48x14 5mm 51 100C UA Low profile separate amplifier RS232 connection O18mm 0 19 20uUm 60mW 100W 48x48x14 5mm 51 100C UAU Low profile separate amplifier USB connection O18mm 0 19 20um 60mW 100W 48x48x14 5mm_ 51 150C SH High power smart sensor O18mm 0 19 20um 60mW 60W 50 8x50 8x33mm 52 150C UA High power built in amplifier RS232 connection O18mm 0 19 20um 60mW 60W 50x50x38mm 52 150C UAU High power built in amplifier USB connection O18mm 0 19 20uUm 60mW 60W 50x50x38mm_ 52 150W UA High power built in amplifier water cooled O18mm 0 19 20um 100mW 150W 50x50x38mm 52 RS232 connection 150W UAU High power built in amplifier water cooled O18mm 0 19 20um 100mW 150W 50x50x38mm 52 USB connection L150C UA Large aperture built in amplifier RS232 connection 50MM 0 19 20um 0 2W 1 50W 80x80x45mm 53 L150C UAU Large aperture built in amplifier USB connection O50mm 0 19 20um 0 2W 150W 80x80x45mm 53 L250W UA Large aperture built in amplifier water cooled 50mm 0 19 20um 0 3W 250W 80x80x58mm 53 RS232 connection L250W UAU Large aperture built in amplifier water cooled O50mm 0 19 20um 0 3W 250W 80x80x58mm 53 USB connection 10 Q OPHIR 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand Standard OEM thermal sensors 0 5W 300W Sensor Features Aperture Spectral Range Power Range S
218. e ASCII N A Text files soreadsheet compatible ASCII Number of sensors One sensor per One sensor per One sensor One sensor per 4 2 1 sensors One sensor One sensor One sensor supported unit unit for single per unit Can unit per unit Can per unit Can per unit Can per unit Can channel mode combine several combine several combine several combine several combine several Two sensors units with units with units with units with units with per unit for dual software for software for software for software for software for channel mode display of up display of up display of up display of up display of up to to 8 sensors on to8sensorson to8sensorson to8sensorson 7 Quasars on one PC one PC one PC one PC one PC Compatible sensors Supports most Ophir pyroelectric thermal and photodiode sensors Power supply Powered Powered Powered Powered 12V wall cube Powered from Powered from Powered from internal from internal from internal from internal plugs into jack USB USB from internal rechargeable rechargeable rechargeable rechargeable on rear rechargeable battery power battery power battery power battery power battery power supply supply supply supply supply Dimensions 205 x 95x 228 x 195 x 208x 117 x Zoe x 189 x 103 x 7 6x55X 155 x 90 x 96 x 95 x 39mm 54mm 40mm 40mm 33mm 22mm 34mm 36mm Notes a The above refers to the rate for logging every single point in turbo mode Above that rate the instrument will sample points but not log every single point b For pyroel
219. e Rate pps 10kHz 5kHz 900Hz 450Hz 100Hz 250Hz 100Hz 50Hz 40Hz 20Hz Noise on Lowest Range yJ 0 5 1 6 10 20 30 60 100 100 100 Additional Error with Frequency 2 to2kHz 2 2 to 2 to 1 to 1 1 1 1 2 45 to 750Hz 400Hz 80Hz SkHz Linearity with Energy for gt 7 of full scale 1 5 aE Damage Threshold J cm lt 100ns 0 1 0 8 Tus 0 2 1 300us 2 5 2mMs 6 10 Maximum Average Power W 15 25 with optional heat sink 15 25 with optional heat sink Maximum Average Power Density W cm 20 20 Uniformity over surface 2 over central 50 of aperture 2 over central 50 of aperture Fiber Adapters Available see page 76 ST FC SMA SC ST FC SMA SC Weight kg 025 0 25 Version Part Number Standard Sensor 7Z02936 7Z02934 StarLink Sensor Direct USB link to PC p 75 787155 787153 Note a Calibration curve is verified and adjusted at specified wavelengths Specified wavelengths 248 266nm 355nm 1064nm and Specified wavelengths 193nm 248 266nm 355nm 532nm 2940nm 1064nm and 2940nm At other wavelengths there may be an additional error up to the value given Max additional error at other wavelengths 2 Max additional error at other wavelengths 2 Note b For wavelengths below 600nm derate damage threshold to 60 of given values Below 300nm derate to 40 of given values Note c With the user threshold setting set to minimum For other settings the spec is for gt 7 of full scale or greater than twice the user thr
220. e and Activex controls are provided StarLab Software Selected Screens Standard Power Screen Digital Power Screen and Color Functions Sensor type and S N FAREL er Saad a Ns Choice of bright on dark or dark on bright characters AARE EL Let ET m Optimize colors for use with laser eye protection glasses Choice of bright on dark or dark on m Can average over selected period Useful for unstable lasers bright characters m Bar graph can show max min average in different colors Power range Go to energy screen Energy Zoom Offent Helj Detailed help Zoom bar graph Subtract can show max min ave offset BeamTrack Power Position Size Screen BeamTrack Power Position Size Screen Monitoring of laser beam size Sensor type and S N Sg 383040 HK Mescurermeni m Accurate tracking of beam position to fractions of a mm parameters B ie d d Power eam position and wander AeA AE a All the other features of standard power energy meters NE EE size graph measurement with BeamTrack sensor Soft Keys OU OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Bran Analog Power Screen m Perfect for adjusting and maximizing laser power m Persistent graphical display allows tracking of minimum maximum values measured m Large analog needle with small digital display as well Choice of smaller display with range men
221. e and user must send reflected energy into appropriate dump A direct back reflection may cause laser cavity to oscillate or if not properly directed may cause damage User must handle all back reflected energy from laser NanoScan Integrated Software package Software for use with NanoScan under Microsoft Windows 32 Bit version only 2000 Professional XP Professional Vista and windows 7 32 64 operating systems Measurements include spot size position and position difference information and laser profiles Includes peak connect and software control of scan speed for measurement of pulsed and pulse width modulated PWM Software includes ability to capture and record bursts of data and ActiveX automation USB 2 0 controller replaces the PCI bus card and allows NanoScan to interface to USB 2 0 port of laptop or desktop PC Performance of Certificate of Calibration traceable to National Institute of Standards and Testing NIST to better than 3 Pyroelectric Detectors Item Description P N USB NS PYRO 9 5 NanoScan Pyroelectric Detector 9mm aperture 5micron slits High resolution head featuring PH00025 pyroelectric detector 63 5mm diameter head with rotation mount 9mm entrance aperture and matched pair of 5um wide slits Use for wavelengths from 190nm to gt 20um This model does not include a cooling fan USB USB NS PYRO 9 25 NanoScan Pyroelectric Detector 9mm aperture 25micron slits High resolution head featuring PH00228 pyroe
222. e best able to satisfy customer requirements Many configurations possible An OEM solution is usually needed to monitor laser performance in the system and possibly to provide fast feedback for system control Depending on your application various configurations can be used such as Simple sensor with raw analog output 1 1 5 Qxelatseas Sensor with electronics providing an analog or digital output Complete instrument including numeric display and or PC interface Custom designed solution for special requirements In the following pages you will see a range of standard OEM sensors available these are actually families of existing OEM sensors with typical specifications shown They can be tailored as needed to fit your specific requirements In addition to the products described below Ophir has developed hundreds of other OEM solutions Simply contact your Ophir representative who is likely to have just the right solution to your needs 2 OPHIR 01 08 2013 ie For latest updates please visit our website www ophiropt com photonics MT TT orporatio Thermal OEM Sensors Ophir pioneered the compact self contained laser power meter sensors with built in amplifiers These sensors are easy to install and give a calibrated voltage proportional to power They contain all the electronics needed including a speed up circuit to increase the speed of response of the sensor to the order of 1s 0 95 Connections to t
223. e connected directly to an oscilloscope via the BNC p Scattered light ee Volume absorber Si photodiode Removable filter connector enabling it to measure the temporal pulse shape of the beam to a resolution of ns Combining the average power measurement with the relative pulse energy and repetition rate the unit calculates the absolute energy per pulse Incoming Laser Beam OU OPHIR __ Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Absorption and Damage Graphs for Pyroelectric Sensors Absorption vs Wavelength 90 00 BB Pyro 80 00 H Pyro metallic 70 00 1 3 RENKON 60 00 PE50 DIF 50 00 ABSORPTION 40 00 30 00 20 00 Pyro metallic 10 00 0 00 0 1 1 0 10 0 WAVELENGTH um Damage Threshold vs Pulse Width 10000 Pulsed Laser Damage Threshold BF 1000 E 100 S Pyro metallic amp D O D 10 QO Pyro BB gt D O c Lu 1 BF 0 3 Pyro BB 0 1 Pyro metallic 0 01 1E 10 1E 09 1E 08 1E 07 1E 06 0 00001 0 0001 0 001 0 01 0 1 1 Pulse Width in Seconds 2 OPHIR cee For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand rt Corporation Bra Wavelength Range and Repetition Rate for Energy Sensors Wave
224. e true 3 dimensional profiles of LEDs providing a 130 degree PH00199 measurement around the source with 0 05 degree resolution LED profiler w 3180 Same as above but includes state of the art PC running Microsoft Windows operating system with Photon LED PH00200 Software installed Configuration required for international sales 3D LED 3 D scan module for LED Profiler PH00207 3LED Mount Standard LED mount for use with packaged LEDs Price dependent on configuration Must be quoted for PH00211 specific device 3CustomFxt Photon can provide custom and semi custom device mounts for LED devices including TE cooled vacuum PH00214 chucks for bare chip testing Mounts are designed to take advantage of the 260 degree field of view available in the LED Profiler Mounting hardware that is compatible with automated test operations can also be designed and supplied by Photon UV Allows the use of the LED Profiler with sources emitting at wavelengths below 380nm PH00212 _ PO Pulsed Operation for LED Profiler PH00213 HIR Y Photonics A Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics Photon OPHIR Photonics A Newport Corporation Brand Product index Product P N Page 1CustomFxt PHOO217 210 LP PHOO201 210 1st Wedge Beam Splitter sPZ17015 177 1W Mount PH00215 210 1X UV image converter SPZ17023
225. ead of analog voltage Possible configurations of thermal OEM solutions include Disc with raw analog output Disc with separate amplifier board Sensor with either raw or amplified analog output m Sensor with RS232 interface m Sensor with USB interface Complete solution including sensor and meter 01 a 2 O HIR __ Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand 1 1 5 1 Standard OEM Thermal Sensors A Newport Corporation Brand Newport Corporation Brand 10mW to 20W Features 20C SH 20C A 20C UAU m Conduction cooled Spectrally flat A version gives analog voltage calibrated to power A m UA version can give analog voltage output or digital RS232 output and can measure power or energy Can also have multiple switchable ranges a9 and or multiple switchable wavelengths Y UAU version is similar to the UA version but operates via the USB terminal of the PC Lf These specifications refer to standard OEM sensors and are to be understood as generic describing sensor families Ophir will be happy to ane help you with a specific solution for your particular application _ Model 20C SH 20C A 20C UAU Type Smart sensor Analog OEM sensor Digital USB connection digital output Features Compact smart senso
226. eads are available to measure CW and pulsed beams across the entire spectral range from UV to far infrared Q OPHIR Photon Photonics For latest updates please visit our website www ophiropt com photonics a Oe eines 01 08 2013 A Newport A Newport Corporation Brand Brand A Newport Corporation Brand 3 3 1 UxSeiaawalarcinais 160 01 08 2013 See Your Beam As Never Before The Graphical User Interface GUI of NanoScan is new Dockable and floatable windows plus concealable ribbon tool bars empower the NanoScan user to make the most of a small laptop display or a large multi monitor desktop PC Simple docked view Measured Beam Results From 1989 through 1996 John Fleischer past President of Photon Inc chaired the working laser beam width ISO DIN committee that resulted in the ISO DIN 11146 standard The final approved standard available in 13 languages is a compromise based on many years of work by the committee The standard governs profile measurements and analysis using scanning apertures variable apertures area sensors and detector arrays NanoScan measures spatial beam irradiance profiles using scanning slit techniques The standard NanoScan uses the moving slit method approved by International Standard ISO DIN 11146 Results measured include Beam Width at various clip levels m Centroid Position m Peak Position m Fllipticity m 1D Gaussian Fit m Beam Divergence m Beam Separatio
227. ecess Phosphor coated 1550nm sensor Comes with USB cable and 3 ND filters BGE USB L11059 BeamGage Enterprise Edition software software license 35mm format 4008x2672 pixel camera Comes SP90321 with universal power supply USB cable and 3 ND filters BGE USB XC1 30 BeamGage Enterprise Edition software software license 320x256 pixel InGaAs camera with C mount SP90251 recess 9 to 1 7um spectral band Comes with universal power supply USB cable external trigger cable and 3 ND filters consult factory for other camera options BeamGage Enterprise Gig E Beam Profiler Systems camera and software BGE GigE OSI182000 BeamGage Enterprise Edition software software license 1 1 8 format 1600x1200 pixel Gig E camera with SP90269 17 5mm C mount CCD recess Comes with Cat5e cable power supply with ext trigger adapter Ethernet destop and laptop PCI Express cards and 3 ND filters BGE GigE OSI182000 1550 BeamGage Enterprise Edition software software license 1 1 8 format 1600x1200 pixel Gig E camera with SP90272 17 5mm C mount CCD recess Phosphor coated 1550nm sensor Comes with Cat5e cable power supply with ext trigger adapter Ethernet destop and laptop PCI Express cards and 3 ND filters Y OPHIR Q Spiricon gt Photonics For latest updates please visit our website www ophiropt com photonics E E UES 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand Newport Corporation Brand Orderin
228. ecifications 4X UV Image Reducing Converter 1X UV Image Converter 4X Beam Expander with UV converter Beam Reduction AX reduction 2 with included 1 1 imaging 2 with included 4X expansion 2 with included lt L correction factor correction factor correction factor Resolution 50um x 50um 35um x 35um 15um x 15um Spectral range 193 to 360nm 40 Minimum signal 1 J cm with blank filter dW Saturation intensity 30mJ cm at 193nm 15mJ cm at 15mJ cm 2 at 193nm 20mJ cm at 30mJ cm at 193nm 15mJ cm at aa 248nm with included filter 20 times above 248nm with included filter 20 times 248nm 20 times above values with values with optional beam splitter greater with optional beam splitter optional beam splitter N Effective Aperture 30mm but effective beam size is 18mm but effective beam size is 1 4 the size of the CCD dimensions F limited to 4X CCD dimensions limited to CCD dimensions 5 Damage threshold 100W cm or 2J cm with beam splitter M Dimensions 50mm dia x 185mm length 31mm dia x 120mm length O29mm dia x 69mm length Ordering Information Item Description P N 1X UV image converter Screw on imaging telescope that converts UV image to visible and images same size on CCD For beam intensities SPZ17023 from 50uJ cm2 to 15mJ cm2 Fits 4 5mm recess and CS mount cameras Beam splitter for above 45 degree wedged beam splitter to reduce intensities on image converter by 20X For beam intensities of up to 300mJ cm 2 at 193nm SPZ17015
229. eclanguiat ar err Play hhg haie died ne D j Bhiasani emrt Busa iiih T ms Energy mind Fiti Eneng AE r Frie Din T r ki ri oe Gplkonal for Best Srann j Winne a Max Width Maea Mia Depth Denbo She ii When the program is started the above screen appears In Step 1 Select the laser type CW or pulsed the beam type circular or rectangular and whether you wish to measure both power and energy or just laser power 2 In Step 2 Enter the required laser parameters beam diameter wavelength max min power or max min energy rep rate and pulse width If minimum power is not entered then the program assumes the minimum is 2 the maximum If desired enter these optional criteria exposure time the maximum time the sensor measures at a time If you only plan to measure the laser power for short periods at a time Ophir offers more compact sensors for intermittent use Sensor size only sensors smaller than the specified dimensions will be selected OU OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand 3 In Step 3 click Find Sensor 4 The sensors that meet specified criteria will be listed in the output screen shown below The sensor type and how close to the damage threshold are listed for each result The input parameters are listed on top 5 In order to find compatible displays click Meter
230. ectric sensors maximum guaranteed baud rate is 9600 c The low cost StarLite power meter does not have a PC Interface support or onboard logging For customers that need these features please consider one of our other offerings 104 Y O HIR 01 08 2013 __ Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand 2 3 Software Solutions 2 3 1 StarLab StarLab turns your PC into a laser power energy multi channel station Extensive Graphic Display of Data m Line Plot Histogram Bar chart Simulated Analog Needle Multiple data sets on one graph or separate graphs on the same screen Advanced Measurement Processing m Power Energy Density Scale Factor Normalize against a reference Multi channel comparisons m User defined mathematical equations channels A B A B C etc m Position amp size measurement with BeamTrack sensors 1 Data Logging for Future Review a m Can be displayed graphically or saved in text format Q Easily exported to an Excel spreadsheet Fully supports Vega Nova ll Pulsar Juno USBI and Quasar devices with all standard Ophir sensors D Flexible Display Options with StarLab Each sensor displayed separately z Fo gt an eo a DOO Q Choose which channels to display Then choose separate or together Maximize one of the sources e ae N oi aeeoa wa ck che jja a at Ser Tea ra Tinapa biketa unslPEe
231. el New Technology 972 3 679 2054 ee Israel Ophir Optronics Ltd 972 2 5484444 E i Italy Ophir Photonics 972 2 5487414 yoram shalev ophiropt com e e e Korea SOLEO CO LTD 82 31 420 2742 sales4 eotechnics com Korea Jinsung Laser 82 42 823 5300 jisukkim jinsunglaser com e o Latvia Optilas Ltd 371 29 781 582 info optilas lv e Lithuania Vildoma 370 5 236 3656 ginutis vildoma lt e e e Malaysia Inno V Global 65 6296 1217 daphne innov global com e e Malta Suratek Ltd 35 621 574 385 ktech1 maltanet net Norway Ophir Photonics 972 2 5487414 yoram shalev ophiropt com e e Poland Lasotronix 48 50 010 0131 mp lasotronix pl o Portugal Ophir Photonics 972 2 5487414 yoram shalev ophiropt com o e o Romania Electro Total 40 21 252 5781 office electro total com Russia Crystaltechno Ltd 7 495 234 5952 chesnokova crystaltechno com Singapore Inno V Global 65 6296 1217 daphne innov global com e Slovakia Kvant spol s r o 421 2 6541 1344 Milan Grigel kvant sk e Slovenia EXTREME d o o 386 1 500 7113 stefanic extreme slo com e South Africa Hitech Laser Systems 27 12 349 1250 hls hitechlasers co za G e s Spain Ophir Photonics 972 2 5487414 yoram shalev ophiropt com e Sweden Ophir Photonics 972 2 5487414 yoram shalev ophiropt com Switzerland Ophir Spiricon Europe 49 4102 6671 802 juergen reingruber eu ophiropt com o Taiwan Unice E O Services Inc 886 3 462 6569 brianh email unice c
232. elength standard 1064nm Others on request Notes b There is a trade off between repetition rate sensitivity and maximum pulse width If standard products are not suitable these parameters can be tailored to customer requirements PE50 S PESOBB S GAG ADJUSTABLE 108 157 Q OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand 1 3 7 2 Examples of Custom OEM Energy Sensor Solutions In addition to the standard OEM products described above Ophir has accumulated over 25 years experience in developing products which are tailored to precise physical configurations provided by the OEM customer These products include special antireflection coatings for specific wavelengths specially configured pyroelectric sensors with or without electronics and much more A number of these special OEM products are shown below lt OEM Pyroelectric Sensor with Built In Amplifier a9 This sensor requires a compact cylindrical case with detector Y sensitivity reaching the diameter edge The 32 x 30mm device has a built in amplifier gt ee Ophir Pyroelectric Sensor with add on OEM Electronics Module This pyroelectric sensor is designed to be used as a Smart Sensor compatible with Ophir Smart meters but also comes with an OEM I F module providing calibrated analog voltage output to host system PE10 OEM Sensor This is a h
233. ely recognize beam characteristics that affect laser performance and operation This instantly alerts you to detrimental laser variations Instantaneous feedback enables timely correction and real time tuning of laser parameters For example when an industrial shop foreman saw the CO laser beam profile in Figure 1 he knew immediately why that laser was not processing materials the same as the Fig 1 Industrial CO laser performing Fig 2 Industrial CO laser performing other shop lasers with the profile shown in Figure 2 inconsistent processing specifed processing Pulsed and CW Lasers The Pyrocam IIl measures the beam profile of both pulsed and CW lasers Since the pyroelectric crystal is an integrating sensor pulses from femtosecond to 12 8ms can be measured The pyroelectric crystal only measures changes in intensity and so is relatively immune to ambient temperature changes Because CW laser beams must be chopped to create a changing signal the Pyrocam III contains an integral chopper as an option 3 2 4 ERRIME Y OPHIR Y Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand n Brand A Newport Corporation Brand ort Corporation Brand Measuring Terahertz Beam Profiles Spiricon s Pyrocam III pyroelectric camera is an excellent tool for measuring THz lasers and sources The coating of the crystal absorbs all
234. entrance iris Requires a Pyro NanoScan System OD OPHIR Photon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand NanoScan Configurations Slits Scanhead Size Detector Type Power Range Wavelength Aperture Silicon 100nW 100mMW 190nm 950nm 25mm Germanium 1uW 100mW 700nm 1800nm 12mm Pyroelectric 100mW 100W 200nm gt 2 0um 9mm 20mm 25um 25um SuM 25mm 25um 100mm 100mm 63mm 100mm The power that can be handled by the IVanoScan is depencent on the wavel2ngth of the light to be measured The wavelength of light determines both its reflectivity from the slit surfaces and the energetic nature of the interactio 1s with materials As a rule of thumb there are three basic wavelength regimes tha govern how much power the scanh 2ad can handle m 3um to FIR gt 20 1m 100W maximu n pyroelectric detector m 700nm to 3umM 25W maximum pyroelectric detector 1W germanium detector 190nm to 700nm 3W maximum pyroelectric detector 1W silicon detector Power levels above these for any of these wavelengths can be considered High Power See the High Power NanoScan section for appropriate products Consult the damage thresholds charts found in the manual before placing an order or exposing any NanoScan slit profiler to a laser beam Q OPHIR __
235. enuator uses the same C mount thread as the other components so it can be combined with additional stackable filters and beam splitters if necessary as shown Illustration of mounted with additional filter and beam splitters Beam Splitters Additional filter Push Pull to vary attenuation Specifications Item Variable attenuator Nominal ND vis 1 6 continuously variable Aperture O20mm Optical quality 2 waves in visible Damage threshold 5W cm 1J cm for ns pulses variable attenuator Attenuation Sliders Transmission Spiricon variable atenuator transmition vs wavelength OU OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics Ca 1050 950 850 750 650 550 450 350 N e max trans m min rtans D O WU aa MM 169 Spiricon OPHIR Photonics 01 08 2013 A Newport A Newport Corporation Brand Brand ATP K Variable Attenuator This option makes beam profiling easy The ATP K attenuates your laser without ghost reflections or fringes and has a knob operated variable wedge attenuator of ND 1 7 4 6 and comes with a fixed gray glass attenuator with ND 2 8 The ATP K is also designed to be used with the HP XXX high power attenuators and beam splitters Both types of attenuators attach directly to the ATP K via C mount The ATP K has simple reproducible attenuation
236. ependent on beam size and scan rate USB 3 8 1 EERIE NH PYRO 9 5 Head only NanoScan Pyro 9mm aperture 5um slits PHOO041 _NH PYRO 9 25 Head only NanoScan Pyro 9mm aperture 25um slits PH00243 NH PYRO 20 25 Head only NanoScan Pyro 20mm aperture 25um slits PHO0042 NH HP NS 20 10 Head only High Power NanoScan 20mm aperture 10um slits PH00043 NH HP NS 9 5 Head only High Power NanoScan 9mm aperture 5um slits PH00044 a Q OPHIR Photon es Photons For latest updates please visit our website www ophiropt com photonics OREN Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand 3 8 2 High Power Laser Profiler Kits for Nd YAG A portable solution for medium power lasers Up to 500W Nd YAG Up to 31mm beam widths 16mm 1 e2 width Easy operation level set and shoot Optimize beams in real time Diagnose problems quickly The LPK YAG Beam Profiler Kit consist of an A R coated reflecting wedge ND filters beam telescope to reduce larger beams a CCD camera and BeamGage software The kit is designed to be conveniently placed in a horizontal beam or under a down directed beam to measure raw beam characteristics amp stability The user must safely handle the 90 to 98 of the beam that passes through the wedge A PC style computer is required but not included See the BeamGage section for software features and calculations See the camera section for specifications LPK
237. era and BeamGage for these wavelengths to give you the best measurements A TA gt av Cc 1440 1605nm i W SA N N Model SP503U 1550 SP620U 1550 Spectral Response nm 1440 1605nm 1440 1605nm M Application NIR wavelengths 1 2 format NIR wavelengths 1 1 8 low resolution format low resolution adjustable ROI and binning Pixel spacing 9 9um X 9 9umM 440um X 4 40um Number of Elements 640 x 480 1600 x 1200 Interface Style USB USB Windows 05 support Windows 7 32 64 Vista 32 64 or XP 32 Pro Despite the small pixel size the spatial resolution will not exceed 50um due to diffusion of the light by the phosphor coating 136 Y OPHIR Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand Software Specifications Features BeamMlc Laser Beam Analyzer Software Features Overview Quantitative Calculations Basic Results Power Energy Results Spatial Results 2D Features 3D Features Statistical Analysis Features Designed for entry level or basic profiling needs Supports our patented Ultracal algorithm plus Auto setup and Auto exposure capabilities Extensive set of ISO quantitative measurements Support for high and low resolution USB cameras Simultaneous 2D and 3D displays Multi instance multi camera use Supports S
238. ergy levels Test plates with same absorber coating as the sensor For testing that laser beam is not above damage threshold 1such plate is included with sensor package The adapter plugs between the Nova D15 socket and the smart plug of the PE C sensor to allow the Nova to operate with PE C series sensors See PE C spec sheet for details The newer PE C series sensors have a p62mm diameter The older PE series sensors have a 85mm diameter This adapter allows using the PE C type sensors in jigs and setups that were originally designed for PE sensors Glass slide 75x25mm with phosphor coating 25x50mm that visualizes spectral region 810 860nm 900 1100nm and 1500 1600nm Stands up to 1KW cn and 0 5J cm Self actuating does not need charging from light source Damage Threshold Test Slides PE C to PE Size Adapter 7208268 IR Phosphor Glass in tasar pi 1 PE C Sensor 7 paipa 7 a Size Adapter Accessory Description Part number Shock Absorbing Post with rubber encased thread to isolate sensor from Metallic type BF type 7EQ6031A 7E06031D TAOS 7208273 TOUS Q OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics 1 3 6 1 Bielaselss 77 01 08 2013 1 3 6 2 Fast Photodetector Model FPS 1 Features Fast 1ns response time Measure temporal pulse shape of short or long pulses Wide spec
239. ers with an additional adapter Ophir P N 7Z08272 see page 77 The adapter can introduce up to 1 additional measurement error The user threshold feature allows adjustment of the internal threshold up to 25 of full scale if desired to avoid false triggering in noisy environments The user threshold setting represents the approximate minimum energy for pulse widths below 50 of the pulse width setting For longer pulse widths the actual minimum may be higher For highest accuracy it is recommended to zero the sensor against the meter the first time it is used with a particular meter For further information see the FAQs on our Website Notes c With the Laserstar Pulsar USBI Quasar and Nova Orion with adapter only 2 of the 5 pulse width settings are available For the PE50 DIF ER C the 30us and 1ms settings and for the PE100BF DIF C the 1ms and 10ms settings Notes d A shock absorbing mounting post is available for situations in which sensor is mounted on a surface subject to shock or vibration This can prevent false triggering and allow working at lower minimum energies Note however that in this case the maximum average power will be reduced to 13W without heat sink and 25W with heat sink see accessory pages 76 77 for heat sink and mounting post Not available for model PE100BF DIF C PE50 DIF ER C PE100BF DIF C Fen i Pas Bha He 4 fig All oa Ct Assembly ADJUSTABLE 122 170 a cee l 75 L 100 i lt Q OPHIR 01 08 2013 Photoni
240. es that are compatible with various sensors click Meter Finder or PC Interfaces Note that some of the newer sensors such as the Pyro C line sensors are only compatible with the newer meters and PC interfaces 01 08 2013 _ 2 OPHIR Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand General Introduction Types of Power Energy Sensors Power and Single Shot Energy Sensors Ophir provides two types of power sensors Photodiode sensors and Thermal sensors Photodiode sensors are used for low powers from picowatts up to hundreds of milliwatts and as high as 3W Thermal sensors are for use from fractions of a milliwatt up to thousands of watts Repetitive Pulse Energy Sensors sensor section section 1 3 Thermal Sensors reading over the surface or better information on the BeamTrack sensors please see section 1 2 Q OPHIR Photonics N Thermal sensors can also measure single shot energy at pulse rates not exceeding one pulse every 5s O N For higher pulse rates Ophir has pyroelectric energy sensors able to measure pulse rates up to tens of kHz These are described in the energy O _ The thermopile sensor has a series of bimetallic junctions A temperature difference between any two junctions causes a voltage to be formed between the two junctions anaes Since
241. escription P N Model USB NFP 1550 NS Model NFP 1550 NanoScan system with Germanium Detector 9mm Aperture 5um Slits High PH00229 resolution 63 5mm diameter head with rotation mount Use from 700nm to 1 8microns Model USB NFP 980 NS Model NFP 980 NanoScan Germanium Detector 9mm Aperture 5 0micron Slits High resolution PH00230 63 5mm diameter head with rotation mount Microscope Objective Lens Mount with 60 1 optics for l 700 1100Nnm l Model USB NFP VIS NS Model NFP VIS NanoScan Silicon Detector 9mm aperture 5um slits High resolution 63 5mm PH00231 diameter head with rotation mount Microscope Objective Lens Mount Bracket with 60 1 optics for 400 700nm Model USB NFP Pyro NFP NS Pyro NanoScan pyroelectric detector with 9mm entrance 5um slits Use for wavelengths PH00232 from 190mm to 20 microns specify wavelengths of use when ordering Lens Mount bracket with well corrected aspheric high energy 60 1 lens with a 0 68 NA Available in wavelengths 400nm 1100nm 3 5 2 RRINE VU OPHIR O Spiricon Photonics For latest updates please visit our website www ophiropt com photonics E 01 08 2013 A Newport A Newport Corporation Brand Brand A Newport A Newport Corporation Brand Brand 3 6 What is M2 M or Beam Propagation Ratio is a value that indicates how close a laser is to being a single mode TEM beam which in turn determines how small a beam waist can be focused For the perfect Gaussian TEM condition the M equals 1 Fo
242. eshold whichever is greater The user threshold is available with Nova Il Vega StarLite or Juno For other meters the threshold is set to minimum and the linearity spec is gt 10 of full scale The PE C series will only operate with Nova or Orion meters with an additional adapter Ophir P N 7Z08272 see page 77 The adapter can introduce up to 1 additional measurement error The user threshold feature allows adjustment of the internal threshold up to 25 of full scale if desired to avoid false triggering in noisy environments The user threshold setting represents the approximate minimum energy for pulse widths below 50 of the pulse width setting For longer pulse widths the actual minimum may be higher For highest accuracy it is recommended to zero the sensor against the meter the first time it is used with a particular meter For further information see the FAQs on our Website Note d A shock absorbing mounting post is available for situations in which sensor is mounted on a surface subject to shock or vibration This can prevent false triggering and allow working at lower minimum energies Note however that in this case the maximum average power will be reduced to 10W without heat sink and 20W with heat sink see accessory pages 76 77 for heat sink and mounting post Note e With the Laserstar Pulsar USBI Quasar and Nova or Orion with adapter only 2 of the 5 pulse width settings are available For the PE C models the 30us and 1ms settin
243. et Zoom Choose analog needle screen Additional Functions Laser tune screen with continuous graph Set startup configuration Power Modes 1 2 EONS AMIGE j Power Configure m Press the menu choice on the Normalize so present Needle Zero l main screen and many more reading is 1 00 Tune Calibrate Adjust sensor i Data Log Response calibration options pop up as shown Enter beam diameter and read i in units of W cm or J cm Put in factor to read input power with attenuator or beam splitter Adjust sensor response time Density Attenuate Limits Adjust power meter Cancel parameters Set for alarm if preset min or max limits exceeded Return to previous menu Specifications Power Meter High legibility 320 x 240 pixel graphics LCD with switchable electroluminescent backlight Large 18mm digits High resolution analog needle also can be chosen Features Many screen features including power with bar graph energy average exposure frequency graphs scaling special units and more Complete on line context sensitive help screens Outputs USB RS232 and 1 2 5 and 10 volt full scale analog output Screen Refresh 15 times sec Case Molded high impact plastic with two level kickstand Size Folds to a compact 208mm Lx 117mm Wx 40mm H Battery Rechargeable NiMH batteries with typically 18 hours between charges The charger can be ordered from your local distributor The
244. etector Position FEto Centered in width 140mm H X 130mm W X 62mm D 35 6mm from bottom 15 2mm behind front cover without included C mount attached Weight MEASUREMENTS PERFORMED BY THE WINDOWS IMAGE VIEWER Total power or energy in digital counts or calibrated in software Peak power or energy in digital counts or calibrated in software Peak location in um 1 52Kg Centroid location in um Diameter at 1 e2 points in um X amp Y Knife edge beam widths in um USING BEAMGAGE Extensive set of quantitative and image display capabilities See BeamGage data sheet FEATURES a 14 bit digital output in CW 13 bit digital output in pulsed a More critical A amp B grading criteria Grade A Up to 50 bad pixels all correctable No uncorrectable clusters Grade B Up to 100 bad pixels No uncorrectable clusters within the 70 central area no more than 2 outside Compact Head 5 53 HX5 13 WX2 53 D Internal integrated focal plane chopper for CW 24 amp 48Hz No separate controller Lens mount and internal focal plane chopper for IR imaging Two Firewire interface ports to PC computer IEEE 1394a OPHIR 2 Photonics A Newport Corporation Brand Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics 2 Spiricon OPHIR Photonics A Newport A Newport Corporation Brand poration Brand 3 2 4 Geeelaawalacliais 153
245. etition rate of the sensor At present only the PE9 F can operate up to 25000Hz b Not including RP sensors PD300 CIE BC20 and PD300 BB Item Description Ophir P N Pulsar 4 Module to operate up to 4 Ophir sensors from your PC USB port Comes with software Max repetition rate for every 7Z01201 pulse 25kHz Has external trigger capability Powered from wall cube power supply can be ordered from your local distributor Pulsar 2 Same as above but for 2 channels only 7Z01202 Pulsar 1 lt Same as above but for 1 channel only 7Z01203 Pulsar USB Cable USB A to B cable 1 unit supplied with Pulsar 7E01202 USB Interface USBI Legacy smart sensor to USB interface with similar performance to Juno but larger size Has analog output See summary 7Z01200 legacy page 104 for specifications 102 o OU OPHIR 01 08 2013 __ Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand 2 2 3 Quasar Wireless Bluetooth Interface Straight from your measuring sensor to your laptop or PC with no cables Quasar table model connects to any Ophir sensor and broadcasts to your PC Wireless range of 10 30 meters depending on surroundings Operates from rechargeable battery with typically gt 40 hours lifetime Powerful USB interface with StarLab PC application software included Converts your PC into a complete laser power energy meter Log power and energy average statistics
246. f the other common industrial lasers Nd YAG and DPSS the upper limits are a little less due to the slightly lower reflectivity of the components at wavelengths around 1000nm Visible and UV lasers can also be measured but these will have lower limits yet The chart below shows the damage thresholds for pulsed beam energies for the three wavelength regimes The lines represent the maximum energies per pulse for various spot sizes that correspond to 5J cm for the 3um to 100um wavelengths 2 5J cm for the 700nm to 3um range and 250mJ cm for the UV Visible range from 190nm to 700nm When operating with pulsed lasers calculate the energy per pulse to ensure that the values fall below these lines for the wavelength of the laser Operation above these values will likely cause damage to the scan head apertures Minimum Beam Size per Pulse Frequency Damage Threshold Curves NanoScan Large Drum HP TO L Rotation Rate Hz 1 25 2 50 5 00 10 00 W Slit Speed um msec 233 25 466 50 933 01 1866 01 100m wae Data Points per Profile 15 13 15 15 lm C Pulse Frequency kHz Minimum Beam Diameter in um m iay lt q 05 6998 13995 N A N A g i 1 3499 6998 13995 N A a tap D 1749 3499 6998 13995 ipd 3 1166 2333 4665 9330 1000 dW 4 875 1749 3499 6998 iin aa 5 700 1400 2799 5598 hp 6 583 1166 2333 4665 ib 10 con 1000 ae 7 500 1000 1999 3999 7 CO 8 437
247. failure mode assessment When questionable pulsed source operation should be verified against CW operation Pulsed Pulsed Upgrade Option to an existing Goniometric Radiometer InGaAs system Failsafe operation for PH00186 InGaAs Upgrade Option pulsed sources operating at repetition rates gt 10kHz with pulse widths gt 500ns For operation below 10kHz there are possible gain saturation states dependent on repetition rate pulse width and source power Consult the factory when operating under these conditions for failure mode assessment When questionable pulse source operation should be verified against CW operation Includes software upgrade Contact Factory for details PCI Controller Upgrade Interface to allow use with standard PCI interface of desktop PC Includes an interface box for 9180 PH00187 controller card PCI Interface card and cable and factory calibration and realignment System should be returned to Photon for installation Includes software upgrade Optional Mount of User Device Photon will provide one semi custom mount of customer s laser diode device Submit device PH00181 LD 8900 Mount particulars for specific quote With this option the instrument can be used immediately and provides one example test fixture LD8900 Software Viewer Goniometric Radiometer Software Viewer for LD8900 models 8 bit Allows users to open review and PH00181 re analyze files that are saved using any PC computer The Viewer has all the data processing feat
248. following specifications refer to standard OEM sensors and are to be understood as generic describing sensor families Ophir will be happy to help you with a specific solution for your particular application L150C UAU Model L150C UA L250W UA L300W UA L250W UAU L300W UAU Type Digital RS232 connection Digital RS232 connection Digital RS232 connection Same as UA but with analog or digital output analog or digital output analog or digital output digital mini USB connection digital output only Features Large aperture built in Large aperture built in Large aperture built in amplifier amplifier water cooled amplifier water cooled Absorber Type Broadband Broadband Broadband Spectral Range um 0 19 20 0 19 20 0 19 20 Aperture mm 50 o 50 50 Power Mode Maximum power 20W free standing 250W water cooled 300W water cooled 150W heat sinked Minimum power 0 2W 0 3W 0 5W Power Noise Level 10mW 15mW 25mW Maximum Average Power Density kW cm2 27 at 20W 12 at 150W 10 at 250W 9 at 300W Response Time 0 95 typ sec 2 5 2 5 2 5 Power Accuracy at calibration wavelength 3 3 3 Linearity with Power 1 2 2 Amplifier power supply for UA UAU versions 6V to 24V 6V to 24V 6V to 24V Via host USB Energy Mode where applicable Maximum Energy 100J 200 3005 Minimum Energy 80m4J 120m4J 200m4J Maximum Energy Density J cm lt 100ns 0 3 0 3 0 3 0 5ms 5 5 5 2mMs 10 10 10 10ms 30 30
249. for long pulses reaching power damage thresholds of up to 100kW cm and 250J cm for 10ms pulses Surface absorbers are suitable for pulses longer than 100us Surface vs Volume Absorbers When measuring a laser with short pulses of tens of us or less the heat is deposited in a short time and cannot flow during the pulse see illustration B below Therefore a surface absorber which absorbs the energy in a thin surface layer is not suitable All the energy is deposited in a thin layer and that layer is vaporized In this case volume absorbers are used These have traditionally consisted of a neutral density glass thermally bonded to a heat conducting metallic substrate The ND glass absorbs the light over a depth of 1 3 mm instead of fractions of a micrometer Consequently even with short pulses where there is no heat flow the light and heat are deposited into a considerable depth of material and therefore the power energy meter with aa volume absorber is able to withstand much higher energy densities up to 10 Joules cm see illustration C These ND glasses form the basis of the Ophir P type absorbers In addition to the P absorbers Ophir has PF and SV absorbers that can stand up to higher average powers and power densities as well as EX absorbers for the UV Long laser pulse gt 100us or continuous Short laser pulse lt 10ps A Surface absorber Heat conducting copper B Surface absorber C Volume absorber or aluminum substrate Laser
250. g Hole 5 5 m 102 6 All Dimensions are in mm IOF Q OPHIR Photon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand Typical NanoScan Operating Space Charts Operating Range is at Peak Sensitivity of Detector Operating Space is NOT absolute THESE CHARTS TO BE USED AS A GUIDE ONLY NanoScan Operating Space Si 3 5mm 1 8um Beam Diameter at 1 e diameter in microns Silicon Detector Silicon Detector Responsivity varies with wavelength Detects between 190 950nm Peak responsivity is 0 4 amps watt at 850nm Detector to detector responsivity variation can be as great as 20 Power Power in the measured laser beam Assumes a round beam diameter An elliptic beam can be approximated by using the maximum width dimension and assuming all the energy is in a beam of this diameter For extremely elliptic beams ratio gt 4 1 contact the factory 3 0 PERIMEVE Pulsed Operation Upper limit of the operating space for pulsed laser measurements Black Coating Removed pyrodetectors are not blackened Slits are blackened to reduce back reflections blackening begins to vaporize near this line Slits in Slit Damage Power density watts cm where one can begin to cut the slits Refer to Photon s Damage Threshold with High Power Laser Measurements docume
251. g Information Item Description P N BeamGage Enterprise FireWire Beam Profiler Systems camera and software BGE FWB GRAS20 DESKTOP BeamGage Enterprise Edition software software license 1 1 8 format 1600x1200 pixel camera with SP90252D 17 5mm C mount CCD recess Comes with 1394b and trigger cable PCI Express interface card and 3 ND filters Desktop model BGE FWB GRAS20 LAPTOP BeamGage Enterprise Edition software software license 1 1 8 format 1600x1200 pixel camera with SP90252L 17 5mm C mount CCD recess Comes with 1394b and trigger cable PCI Express interface card camera power supply and 3 ND filters Laptop model BGE FWB GRAS20 1550 DESK BeamGage Enterprise Edition software software license 1 1 8 format 1600x1200 pixel camera with SP90253D 17 5mm C mount CCD recess Phosphor coated 1550nm sensor Comes with 1394b and trigger cable PCI Express interface card and 3 ND filters Desktop model BGE FWB GRAS20 1550 LAPTP BeamGage Enterprise Edition software software license 1 1 8 format 1600x1200 pixel camera with SP90253L 17 5mm C mount CCD recess Phosphor coated 1550nm sensor Comes with 1394b and trigger cable PCI Express interface card camera power supply and 3 ND filters Laptop model Software Upgrades BEAMSTAR TO BGS UPGRADE Upgrade any BeamStar FX or SP based product to BeamGage Standard Edition Requires a camera key to SP90219 activate SP cameras may require a firmware upgrade to e
252. g Users can subdivide the imager into separate beam measurement regions All enabled results are computed inside of each partition The manual aperture is used to define and create rectangular partition When partitioning is enabled some new results items will be enabled Centroid measurements between beams in each partition can be performed Partitioned imagers must have a single origin common to all partitions All coordinate results are globally referenced to this single origin 3 2 1 4 RECREIO Statistical Analysis Performed on all measurement functions with on screen display a Choices of intervals Manual start stop m Time from 1 second to 1000 hours Frames from 2 to 99 999 Measurements reported Current frame data Mean Standard Deviation Minimum Maximum of each calculation performed Controls integrated with beam stability results scatter and strip chart plots Y OPHIR Y Spiricon Photonics For latest updates please visit our website www ophiropt com photonics E 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand Newport Corporation Brand Features BeamGage Standard BeamGage Professional BeamGage Enterprise all features in Standard plus all features in Pro plus File types Industry Standard HDF5 data and setup file format which are compatable in third party applications such as MatLab and M
253. ge Professional BeamGage Enterprise all features in Standard plus all features in Pro plus Frame Averaging Frame Summing Convolution Adjacent Pixel Averaging Beam Maker Camera Features Camera related features in the applications Trigger Capture and Synchronization Methods less than zero that result from noise when the baseline is subtracted Retaining fractional and negative numbers in the processed signal can increase the beam width measurement accuracy by up to 10X over conventional baseline subtraction and clip level methods Spiricon s Ultracal conforms to the best method described in ISO 11146 3 2004 Up to 256 frames can be averaged for a signal to noise ratio S N improvement of up to 16X Noise is averaged up to 1 256th 8 fractional bits Data is processed and stored in a 32bit format Up to 256 frames can be summed to pull very weak signals out of the noise Due to the precise nature of Ultracal baseline setting i e a retention of both positive and negative noise components summing of frames can be performed without generating a large offset in the baseline Choice of 5 convolution algorithms for spatial filtering for both display and calculations Spatial filtering improves the visual S N Beam Maker is a new feature that allows the user to model both Laguerre Gaussian and Hermite Gaussian laser beams in various modal configurations With these models you have verification and va
254. gent beams 12mm aperture For fiber or free space input Model Use Absorber Type Spectral Range um Aperture mm Maximum Beam Divergence Sensitivity to beam size and angle Power Mode Power Range Power Scales Power Noise Level Maximum Average Power Density kW cm Response Time with Meter 0 95 typ s Power Accuracy Linearity with Power 3A IS 3A IS IRG 3A IS 3A IS IRG Divergent beams to 3W for Divergent beams to 3W for IR visible NIR Integrating sphere with Si Integrating sphere with InGaAs detector detector 0 42 1 1 0 8 1 7 p 12mm p 12mm 40 degrees 40 degrees 2 2 1uW 3W 1uW 3W 3W to 3uW and dBm 3W to 3uW and dBm 20nW 20nW 0 2 on integrating sphere surface 0 2 0 2 5 at 420 1000nm 5 10 at 1000 1100nm Energy Mode Energy Range NA NA Energy Scales NA NA Minimum Energy mJ NA NA Maximum Energy 5mJ 5mJ Maximum Energy Density J cm lt 100ns 0 5 905 0 5ms 6 6 Zip MS 12 12 10ms 25 25 Cooling convection convection Fiber Adapters Available see page 44 SC ST FC SMA SC ST FC SMA Weight kg 0 6 0 6 Version V1 Part number 7Z02404 7Z02403 Notes a One fiber output port available with output 2E 4 of input power mm of fiber area b On integrating sphere surface 3A IS 3A IS IRG 68 46 ALTERNATE POLE 2x M3x6 deep MOUNTING THREAD G12 95 0 137 J ADJUSTABLE 75 1 1 1 3 2 Byaatsevas 27 Q OPHIR
255. ger cables PCI Express interface card camera power supply and 3 ND filters Laptop model BGP FWB GRAS20 1550 DESK BeamGage Professional Edition software software license 1 1 8 format 1600x1200 pixel camera with SP90243D 12 5mm C mount CCD recess Phosphor coated 1550nm sensor Comes with 1394b and trigger cables D PCI Express interface card and 3 ND filters Desktop model A BGP FWB GRAS20 1550 LAPTP BeamGage Professional Edition software software license 1 1 8 format 1600x1200 pixel camera with SP90243L 12 5mm C mount CCD recess Phosphor coated 1550nm sensor Comes with 1394b and trigger cable PCI Express interface card camera power supply and 3 ND filters Laptop model BeamGage Enterprise USB2 Beam m Profiler Systems camera and software N BGE USB SP503 BeamGage Enterprise Edition software software license 1 2 format 640x480 pixel camera with 4 5mm SP90246 CCD recess Comes with USB cable and 3 ND filters M BGE USB SP503 1550 BeamGage Enterprise Edition software software license 1 2 format 640x480 pixel camera with 4 5mm SP90247 CCD recess Phosphor coated 1550nm sensor Comes with USB cable and 3 ND filters BGE USB SP620 BeamGage Enterprise Edition software software license 1 1 8 format 1600x1200 pixel camera with SP90248 4 5mm CCD recess Comes with USB cable and 3 ND filters BGE USB SP620 1550 BeamGage Enterprise Edition software software license 1 1 8 format 1600x1200 pixel camera with SP90249 45mm CCD r
256. gh Power NanoScan can measure focused CO laser beams up to 5 kilowatts The High Power NanoScan is equipped with a pyroelectric detector with copper slits and drum A cooling fan mounted on the scan head body provides additional heat management With the new peak connect algorithm and the software controlled variable scan speed the High Power NanoScan is ideal for measuring lasers operating with pulse width modulation PWM power control Measurement of Q switched lasers and other higher frequency pulsed lasers is also possible using this feature What Can be Measured Measuring high power beams can be tricky The lasers have the potential to damage the scan head and any reflected light can be dangerous to both the operator and the surroundings The High Power NanoScan can measure these beams because it uses a combination of highly reflective components with high thermal dissipation capability It is important to manage the reflected beam so that it neither reenters the laser cavity nor sends stray beams into the surrounding area The scan head is designed to make short duration measurements to avoid excessive heating of components The head should be only in the incident beam for 10 to 60 seconds depending on the power levels to prevent excessive heating of the components The High Power NanoScan scan head has been shown to be able to handle power densities of 3 2WWcm at 10 6um the power density of a 200Um beam at 1kW At the shorter wavelengths o
257. ght kg 0 4 0 8 0 35 0 4 0 4 0 45 Version Part number Standard Sensor 7Z02741 7Z02744 7Z02727 7Z02728 7Z02731S 7Z02733 BeamlTrack Sensor Beam Position amp 7Z07901 Size 0 57 58 Notes a For shorter wavelengths derate Wavelength Derate to value Notes b at calibrated maximum energy density as follows idemie merdasiec wavelengths 755nm 532nm 80 of stated value 1064nm and 532nm only 355nm 60 of stated value Notes e When sensor 266nm 40 of stated value is hot there can be large 193nm NA zero offset up to 300mMW Notes c LP1 sensors have relatively large spectral variation in absorption and have a calibrated spectral curve at all wavelengths in their spectral range to the above specified accuracy Nova and Orion meters do not support this feature and when used with those meters accuracy will be 3 for 532nm 808nm 1064nm and 2100nm and 6 for other wavelengths in the spectral range 400 1100nm Notes d For lower powers up to 30W it is recommended to work with the fan off and then the noise level is 3 times lower It is also recommended to measure energy with the fan off F100A PF DIF 33 F100A PF DIF 18 F150A BB 26 026 iB FL250A BB 35 FL250A LP1 DIF 33 w FL250A LP1 35 035 993 3 i E AI DC Po E 100 36 l wo n OPHIR 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 1 1 2 5 Medium High Power Fan
258. gions with separate results 1D Features Available overlaid with 2D and 3D or in separate windows X any Y plots on separate or combined displays 1D displays with basic results and column row summing option Tophat 1D displays with Tophat results Gaussian 1D displays with Gaussian fit results 1D Profile display of the Gauss fit results on 1D 2D and 3D displays 2D Feie Continuously zoomable and resizable displays in satellitable window Continuous Z axis display magnitude scaling Zoomable to subpixel resolution for origin and cursor placements Pixel boundaries delinated at higher zoom magnifications Adjustable Cursors that can track peak or centroid Adjustable Crosshairs that can track peak or centroid Adjustable manual apertures Viewable Auto aperture placement Displayed beam width marker Integrated Mouse actuated pan zoom controls Separate 2D pan zoom window to show current view in 2D beam display Manual or fixed origin placement Ability to create partitions using the manual aperture controls 3D Features 3D graphics utilize solid surface construction with lighting and shading effects Integrated Mouse actuated pan zoon tilt rotate controls Selectable Mesh for drawing speed vs resolution control Continuously zoomable and resizable displays in satellitable window Continuous Z axis display magnitude scaling User enabled backplanes with cursor projections Partitionin
259. gn with rubberized bumpers and optimized kickstand Choice of digital or analog needle display Analog output Easy to use soft keys Easy measurement configuration with context sensitive help Backlighting and rechargeable battery Single shot energy measurement with thermal sensors Power averaging Resizable Screen graphics EMI rejection StarLite is a low cost power energy meter capable of measuring power or energy from pJ and pW to hundreds of Joules and thousands of Watts It also supports position and size measurement with the BeamTrack family of sensors StarLite can also display the power or energy with a high resolution simulated analog needle display All StarLite measurement screens can be configured to either show the measurement parameters or to hide them in order to maximize the graphical and numeric displays StarLite can be operated either by battery or from an AC source with the charger plugged in at all times Its backlight allows illumination of the power meter in low light conditions Selected Screens Digital Power Screen CW industrial medical and scientific lasers pW to Multi kW with appropriate sensors m Can average over selected period Useful for unstable lasers m Fast response bar chart BeamTrack Power Position Size Screen Monitoring of laser beam size m Accurate tracking of beam position to fractions of a mm m Power measured at the same time 1 5 BROelaleinelas Barchart Display of Po
260. gnal me Linear From Min Signal 3500 3000 2500 2000 1500 Magnitude in Digital Counts Output signal in digital counts 1000 0 100 200 300 400 500 600 Total input Power in uW Non linear output of the 1550 series cameras SP 1550M Camera Comparison of Beam Shape with and without Correction Factor 4000 3500 3000 2500 Beam Width With Correction width 86 Pixels 2000 Without Correction width 58 Pixels 1500 1000 500 0 O 10 20 30 40 50 60 70 80 90 100 110 120 Beam Width in Pixels Cross section of a fiber beam with and without non linearity correction Spiricon VU OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Wavelength Response The anti Stokes up conversion efficiency is very wavelength dependent This graph shows the typical spectral response curve of a new high response coating As seen we have calibrated the response from 1527nm to 1605nm We have extrapolated the shorter wavelength region by comparing our measured response to data published over the entire range Phosphor Coated CCD Response 100 mW cm 2 for Full Video Measured Signal required versus wavelength to achieve Extrapolated from i i i i E ehal este camera full signal illumination by anti Stokes up conversion material
261. gs and for the PE BF models the 1ms and 10ms settings Note f The 3000nm setting is calibrated for 10 6um as well To measure CO laser set to the 3000nm setting The additional error for measuring 10 6um is 5 For sensors drawings please see page 71 Q OPHIR Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand 1 3 3 High Energy Pyroelectric Sensors 20puJ to 10J Features Sensors with diffuser for high energies and high energy densities PE50 DIF C PE25BF DIF C Metallic coating for high rep rates ee BF coating for highest damage threshold Wide spectral range Measure YAG and G harmonics and many more a9 m Rep rates up to 10kHz Y Measure lasers with pulse widths up to 20ms CY TT Model PE50 DIF C PE25BF DIF C Use High rep rate Complete calibration curve Complete calibration curve High damage threshold Aperture mm 035 p20 Absorber Type Metallic with diffuser BF with diffuser Spectral Range um Q19 3 OSs 22 Surface Reflectivity approx 25 25 Calibration Accuracy 2 3 Max Pulse Width Setting 2s 30us 500us Ims 5ms Ims 2ms 5ms 10ms 20ms Energy Scales 10J to 10J to 10Jto 2mJ 10J to 2mJ 10J to 10J to 2mJ 10J to 2mJ 10J to 10J to 10J to 200uJ 200uJ 20mJ 20mJ 20mJ 20mJ Lowest Measurable Energy uJ 8 20 20 100 120 200 100 150 200 200 300 Max Pulse Width ms 0 002 0 03 0 5 5 1 2 5 10 20 Maximum Pulse Rate pps 10kHz
262. gured thermal or photodiode based power sensors and much more A number of these special OEM products are shown below OEM Photodiode Sensor with RS232 Output This sensor is similar to the UA thermal OEM sensors described above except it has a photodiode instead of thermal detector The sensor shown has 5 decades of dynamic range and has the following dimensions 50mm x 50mm x 33mm OEM Photodiode Sensor with Universal Amplifier Board Truncated PD300 sensor with Universal amplifier board giving calibrated voltage output Either analog or RS232 communication 1 1 5 2 Bialawceras Flat Profile Thermal Sensor This sensor with 50mm aperture is used as an exposure detector for photolithography and is only 10mm thick Super Compact Thermal Sensor D Thermal OEM sensor designed to be cemented into user system Dimensions are under i 10mm x 20mm footprint and 4mm height The sensor can be connected to an Ophir smart meter to measure power or energy or can be used directly with voltage output Compact hand held thermal Smart Sensor This thermal sensor is only 20mm thick to enable probing in hard to reach locations and can measure up to 25W It is designed specifically to be hand held and works with any Ophir Smart Meter Ultra Fast OEM Power Sensor Using an innovative new axial thermopile method this sensor is designed to be built into an industrial CO2 or YAG laser for fast feedback to control the laser power stability
263. h PE C series sensors See PE C spec sheet for details Damage Threshold Test Test plates with same absorber coating as the sensor For testing that laser beam is not above damage threshold 1 such Plates plate is included with sensor package There are test plates of the following types Metallic and BF PE C to PE Size Adapter The newer PE C series sensors have a 62mm diameter The older PE series sensors have a P85mm diameter This yi adapter allows using the PE C type sensors in jigs and setups that were originally designed for PE sensors IR Phosphor Card Glass slide 75x25mm with phosphor coating 25x50mm that visualizes spectral region 810 860nm 900 1100nm and 77 1500 1600nm Stands up to 1KW cm and 0 5J cm Self actuating does not need charging from light source Fast photodetector model FPS 1 Accessory Description Page FPS 1 Fast Photodetector Connect to oscilloscope to measure temporal beam profile 1 5ns response time 78 OEM Energy Sensors Standard OEM pyroelectric energy sensors 2yJ 10J Sensor Features Aperture Spectral Energy Max Ave Max Freq Size Page Range Range Power PE10 S Slim profile sensitive no amplifier O12mm 0 19 3um 2uJ 20mJ 2W 400Hz 50 8x14mm 81 PE10 S Q Very compact no amplifier O8mm 0 19 3um 2uJ 20mJ 2W 100Hz 30x40x14mm_ 81 PE25 5 Slim profile med aperture no amplifier 24x24mm 0 19 3um 0 1mJ 10J 10W 40Hz 50 8x14mm 82 PE25BB 5 As above broadband coating 24x24mm 0 19 20um 1mJ 10J 10W 20Hz 50 8x14mm_ 82
264. has been characterized by ever increasing laser powers and energies and increasingly concentrated laser beams Medical industrial and scientific applications of these high power and energy density lasers require reliable and accurate measurement of power and energy Meters for relatively high powers and energies generally operate by measuring the heat deposited onto an absorbing element The key to accurate and reliable measurement is the makeup of this absorbing surface It must stand up to repeated use without degradation or change in calibration Laser sources are constantly growing in power energy and beam concentration Ophir has an ongoing program of development of durable absorbing surfaces that will continue to stand up to the most punishing laser sources as they grow in intensity and Ophir has some of the highest damage threshold absorbers in the industry Ophir Spiricon Photon brings the same leading edge innovation to laser beam profile measurement with its famous Pyrocam its in house designed SP and Nanoscan cameras and BeamGage software Ophir s Laser Measurement Group products are used in three highly competitive and sophisticated fields medical industrial and research Each of these areas is further divided into end users and OEMs Medical Ophir is the largest producer of laser power and energy measurement equipment for the medical market where Ophir s power measurement devices are incorporated into laser based
265. he 4X beam expander is an expanding telescope that images the beam as it looks at 8mm from the end of the expander onto the CCD while enlarging the image 4X In addition to the 4X beam expander other microscope objectives are available for expanding the beam even more There are objectives for 6X 12X and 22X expansion The various expanders allow the use of our 2 and 10 filters as well as the variable attenuator so as to accommodate the camera to a wide range of source intensities With a camera having 4 4um pixel spacing using the beam expander the effective resolution can be as good as 0 5um The object plane that is inaged onto the CCD is located several mm in front of the assembly so even hard to get to focal spots and other small images are easy to image The beam expanders are designed to accommodate up to 3 screw on filters or a variable attenuator behind them so a wide range of intensities can be accommodated For intensities too large to be accommodated by just filters beam splitters are available to reduce the intensity before the beam expander The beam expander is primarily intended for nonparallel Microscope objective assembly beams such as focal spots and fiber tips If small parallel beams are imaged interference effects RENO poate may Occur The 4X Beam expander can also be fitted with a UV converter plate at its object plane so that you can look at small beams in the spectral range 193 360nm and expand them 4x See ordering
266. he LBS 300 beam splitter attachment for C mount CS mount or Ophir mount cameras allow you to measure laser beams with diameters up to 15mm and powers ranging from 10 mWatts to 400 Watts The beam sampler is designed so that the preferential polarization selection effect of a single wedge is cancelled out and the resulting beam image is polarization corrected to restore the polarization components of the original beam The beam sampler operates by reflecting the incoming beam from the front surfaces of a pair of wedges through 90 degrees into the camera Approximately 99 of the beam is transmitted through the beam sampler with 0 01 passed on to the camera A set of adjustable ND filters are provided to make final intensity adjustments to the beam before it reaches the camera imager As an option you may order the WVF 300 P N SP90195 continuously variable ND filter set that can slide in and replace the fixed ND filters If additional attenuation is needed an external wedge P N SPZ17015 may be mounted at the input port however this 3rd wedge will cause polarization selectivity when the beam is significantly polarized different in the S and P planes Alternatively two LBS 300s can be coupled in series providing up to a 108 attenuation Primary beam in Primary beam out Y 2 45 wedges to reflect Selection of 4 adjustable Optional SP90273 Large C mount Wedge Splitter N the primary beam into ND filte
267. he array of thermocouples measures the temperature gradient which is proportional to the incident or absorbed power In principle the reading is not dependent on the ambient temperature since only the temperature difference affects the voltage generated and the voltage difference depends only on the heat flow not on the ambient temperature Since all the heat absorbed flows through the thermocouples as long as the laser beam is inside the inner circle of hot junctions the response of the detector is almost independent of beam size and position If the beam is close to the edge of the inner circle some thermocouples become hotter than others but since the sum of all of them is measured the reading remains the same Generally Ophir specifies 2 uniformity of reading over the surface or better Cold junction 1 1 Wxelaisvelas Output Using Power Sensors to Measure Single Shot Energy Although Ophir thermal power sensors are used primarily to measure power they can measure single shot energy as well where they integrate the power flowing through the disc over time and thus measure energy Since the typical time it takes for the disc to heat up and cool down is several seconds these thermal sensors can only measure one pulse every several seconds at most Thus they are suitable for what is called single shot measurement Although the response time of the sensor discs is slow there is no limit to how s
268. he sensors are simple with the host providing DC power and the sensor providing a voltage output proportional to power In most cases the sensor is used in one of three ways 1 Beam Dump Mode For lasers such as surgical lasers which are used in short bursts the sensor is a beam dump with full power on it at all times except for the short periods of beam use when the beam is deflected to the work area Deflectable Mirror eee ere eer ey eee a 1 1 5 Befelaisvelas To target LASER OEM power meter 2 Sampling Mode In this mode the laser is usually available to the user and is only deflected to the monitor for short times when the beam is sampled by the sensor Sampling is performed with a deflection mirror or with an output fiber optic cable which is inserted into the measuring port from time to time ar To target flexible cable OEM power OEM sensor in meter measuring port 3 Rear Leak Mode In this mode a small fraction 0 5 2 of the laser beam leaks out of the rear mirror of the laser and is constantly monitored by the sensor 0 5 2 gt 98 OEM power o LASER gt To target meter Q OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand Advantages of Ophir Thermal OEM Sensors Compactness Available in sizes down to 38x38x25mm or 48x48x15mm Versatility Oph
269. he standard configuration is supplied with a glass OD 2 8 C mount neutral density filter for wavelengths gt 360nm and an OD 3 0 Fused Silica Inconel neutral density filter for wavelengths lt 360nm Because of the limited usefulness of exposure control with pulsed lasers the Photon Inc Model ATP is recommended for use with pulsed us lasers with repetition rate lt 10kHz and wavelength gt 360nm For pulsed lasers sill with wavelength lt 360nm a variable UV filter or a combination of UV filters will generally be required ModeScan 1780 ModeScan Model 1780 System Specifications Optical Sensor Detector Sensor Si CCD 1 2 Format Wavelength 360nm 1100nm Standard with OD 2 8 filter 250nm 1100nm with UV optics Pixel Array 780 H x 580 V Pixel Size 8 3um Xx 8 3uM Array Dimension 649mm x 4 83MM Scanning Mode Progressive CCD Cover Glass Removed Beam Splitters Fused Silica lt 20 10 Scratch Dig 10 Flatness Test Lenses 200mm fl Fused Silica 250 460nm AR coated standard UV 250 460nm 200mm fl BK7 425 720nm AR coated standard Visible 425 720nm 200mm fl BK7 620 1080nm AR coated standard VIS NIR 620 1080n other fl s optional for all wavelengths Fixed Attenuator Visible NIR OD 2 8 Absorbing Glass gt 360nm UV OD 3 0 Fused Silica Inconel 250 450nm Computer Electrical 01 08 2013 A D Conversion 12 Bit Maximum Frame Rate 35 8fp
270. herefore should not be used whenever it is not necessary to measure the energy of each pulse and average power measurement is sufficient Pyroelectric sensors use a pyroelectric crystal that generates an electric charge proportional to the heat absorbed Since the two surfaces of the crystal are metalized the total charge generated is collected and therefore the response is not dependent on beam size or position This charge then charges a capacitor in parallel with the crystal and the voltage difference thus generated is proportional to the pulse energy After the energy is read by the electronic circuit the charge on the crystal is discharged to be ready for the next pulse The response time of the pyroelectric sensor depends on the time it takes for the heat to enter the crystal and heat it up For metallic type pyro detectors this time is tens of us and thus the metallic type can run at a high repetition rate For the BF and BB type the response time is hundreds of us with a correspondingly lower repetition rate Ophir pyroelectric detectors have unique and proprietary circuitry that allow them to measure long pulses as well as short pulses and work at a high duty cycle i e where the pulse width is as much as 30 of the total cycle time Ophir came out with the new compact C line of pyroelectric sensors that replaced previous models The electronics and mechanics has been completely upgraded and the new sensors are superior in every way more comp
271. hin Profile to 30W O26mm 0 15 20uUm 80mW 30W 20mJ 60J 30 50 150 A BB 26 General purpose to 50W 150W intermittent 26MM 0 19 20um 40mW 150W 20mJ 100J 30 10A P Pulsed lasers up to 10W O16mm 0 15 8um 4OmW 10W 10mJ 10J 31 30A P 17 Short pulse lasers to 30W O17mm 0 15 8um 60mW 30W 40mJ 30J 31 50A PF DIF 18 High energy density pulsed beams 17 5MM 0 24 2 2uM 140mW 50W 60mJ 200J 31 15 50 A PF DIF 18 As above compact for intermittent use O17 5mm 0 24 2 2um 140mW 50W 60mJ 200J 3 30A N 18 High power density pulsed YAG O17 5mm 0 532 1 064um 60mW 30W 30mJ 200J 31 Low medium power thermal sensors apertures 17mm to 35mm 30mW 150W Sensor Features Aperture Spectral Range Power Range Energy Range Page 30 150 A BB 18 CW to 30W intermittent to 150W O17 5mm 0 19 20UmM 30mMW 150W 20mJ 100J 32 30 150 A LP1 18 As above high damage threshold for long pulses and CW 17 5mm 0 25 2 2uM 30mW 150W 20mJ 300J 32 L50 150 A BB 35 CW to 50W intermittent to 150W 35MM 0 19 20um 100mW 150W 40mJ 300J 32 8 OU OPHIR 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand Sensor Features Aperture Spectral Range Power Range Energy Range Page L50 150 A LP1 35 CW to 50W intermittent to 150W high damage O35mm 0 25 2 2UM 100mMW 150W 40mJ 300J 32 threshold for long pulses L50 150 A PF 35 CW to 50W intermittent to 150W for short pulse lasers 35mm 0 15 20UmM 100mMW 150W 50mJ 300J 32 30
272. hin the claimed limits of linearity The Comet 10K series measures the heat rise of the absorbing puck when irradiated by the laser for 10s In order to calibrate the Comet 10K we simply irradiate with a lower power laser for longer e g 150W for 60s Thus the heating effect is similar to that of a higher power laser Tests of the Comet calibrated by this method vs NIST traceable high power sensors has shown that it is accurate and reproducible For more information on calibration please see our website at www ophiropt com calibration procedure tutorial Photodiode Sensors A photodiode sensor is a semiconductor device that produces a current proportional to light intensity and has a high degree of linearity over a large range of light power levels from fractions of a nanowatt to about 2 mW Above that light level corresponding to a current of about 1mA the electron density in the photodiode becomes too great and its efficiency is reduced causing saturation and a lower reading Most Ophir PD sensors have a built in filter that reduces the light level on the detector and allows measurement up to 30mW without saturation Most sensors have an additional removable filter allowing measurement to 300mW or 3 Watts depending on the model Principle of Operation When a photon source such as a laser is directed at a photodiode detector a current proportional to the light intensity and dependent on the wavelength is created Since many low power lasers ha
273. hort the pulses measured are since the measurement is of the heat flowing through the disc after the pulse Beamtrack Power Position Size sensors Ophir now has the new BeamTrack thermal sensor that can measure beam position gnd 3st and beam size as well as power This innovative device provides an additional wealth of Quad information on your laser beam centering beam position and wander beam size as well as power and single shot energy The BeamTrack sensor is illustrated schematically here and works as follows the signal coming from the sensor is now divided into 4 quadrants so by measuring and comparing the output from the 4 sections we can determine the position 1st of the center of the beam to a high degree of accuracy In addition to the 4 quadrants Quad there is now a special proprietary beam size detector After processing outputs from these Beams various detectors the user is presented with the beam position as well as beam size Note detector that the beam size is calibrated only for a Gaussian beam of gt 3mm but for other beams it will give relative size information and will indicate if the beam is changing size For more 4 Quad Total output information on the BeamTrack sensors please see section 1 2 Types of Thermopile Discs There is no single absorber which meets the needs of all applications Ophir has developed several types for different applications such as long pulses
274. hs 2 format low resolution mat low resolution adjustable format adjustable ROI ROI and binning Spectral Response 1440 1605nm 1440 1605nm 1440 1605nm 1440 1605nm Maximum beam size 6 3mm W x 4 7mm H 7 1mm W x 5 4mm H 7 1mm x 5 4mm 4 7mm x 5 4mm Pixel spacing 9 9umM x 9 9umM 44um x 4 4um 44um x 4 4um 8 4umM x 9 8umM Number of effective pixels 640 x 480 1600 x 1200 1600 x 1200 640 x 480 pixels Minimum system 30 dB 30 dB 30dB 30dB dynamic range Linearity with Power 5 5 5 5 Spatial Uniformity 5 5 5 5 Accuracy of beam width 5 for beams larger than 0 6 mm Frame rates 30 fps at full resolution 8 fos at full resolution 15Hz full res 30 Hz In 12 bit mode 60 fos at 320x240 28 fos at 640x480 gt 60Hz with smaller ROI 44 fos at 320x240 Shutter duration 30us to multiple frame times 1 60 to 1 100 000 sec 9 steps Gain control 43 1 manual 29 1 manual Odb to 25db Manual control Manual adjustment Trigger Supports both Trigger In and Strobe Out N A Photodiode trigger Consult Factory N A consult factory N A Saturation intensity 7mW cm at 1550 nm Lowest measurable signal 50uW cm2 Damage threshold 50W cm 0 1J crm2 with all filters installed for lt 100ns pulse width 70 mW cm 2 at 1550 nm 70 mMW cm at 1550 nm Dimensions and CCD 96X76X16mm 4 5mm below 96X76X28mm 4 5mm below 20mm x 44mm x 58mm Fixed 37mm x 34mm x 56mm CCD recess Surface Surface C mount recess from surface 12 5mm Adjustable Operation mode Interline tran
275. hts below 600nm derate damage threshold to 60 of given values Below 300nm derate to 40 of given values Note c For gt 7 of full scale with the user threshold setting set to minimum For other settings the spec is for gt 7 of full scale or greater than twice the user threshold whichever is greater The user threshold is available with Nova Il Vega StarLite or Juno For other meters the threshold is set to minimum and the linearity spec is gt 10 of full scale The PE C series will only operate with Nova or Orion meters with an additional adapter Ophir P N 7Z08272 see page 77 The adapter can introduce up to 1 additional measurement error The user threshold feature allows adjustment of the internal threshold up to 25 of full scale if desired to avoid false triggering in noisy environments The user threshold setting represents the approximate minimum energy for pulse widths below 50 of the pulse width setting For longer pulse widths the actual minimum may be higher For highest accuracy it is recommended to zero the sensor against the meter the first time it is used with a particular meter For further information see the FAQs on our Website Note d A shock absorbing mounting post is available for situations in which sensor is mounted on a surface subject to shock or vibration This can prevent false triggering and allow working at lower minimum energies see accessory page 77 for mounting post Note e The 3000nm setting is
276. i e f PE api ER h EPET E En 1 4 Strip chart of beam D4sigma width Note how changing conditions affects the width repeatability Beam intensity changed over 10db making noise a significant factor in measurement stability Beam Pointing Stability Open the Pointing Stability Window to collect centroid and peak data from the core system and display it graphically View a chart recorder and statistical functions in one interface na n rim oe ff bi e a ansa ee ee ee TEST E ee eee aIMl hee oe I m E p m ye aa r s A ag Paint af in Peak location scatter plot with histogram color coding 20 en ie ED eee See fo uer am AE i Foot E x we i A centroid location scatter ten Jae plot with histogram color Pami 5a a gt coding Le ie pee a eeeeeee SS Set a sample limit and specify the results items to graph on the strip chart i L eel W E p EET A pointing stability strip chart ba thn shi octal A presents data over time for The radius is referenced from the Centroid X and Y Peak either an Origin established pepe ee ee eye ee sa X andY and centroid radius in BeamGage or from the ms ere i hiii from an origin or from the continuously calculated wee atini aaa iaa daa sahani siani dieiis Mik aa dih hah hha i he en dl ci mean centroid Average Centroid position ST nas as Easy to Use and Powerful BeamGage is the
277. icon photodiode 010mm 0 19 1 1 um 1nJ 20uJ 20 000Hz 65 PD10 pJ C Lowest energies down to pJ Silicon photodiode 010mm 0 2 1 1um 10pJ 200nJ 20 000Hz 65 PD10 IR pJ C Lowest energies down to pJ Germanium photodiode O5mm 0 7 1 8umM 30pJ 20nJ 10 000Hz 65 Pyroelectric energy sensors 0 2yJ 10J Sensor Features Aperture Spectral Range Energy Range Maximum Frequency Page PE9 C Pyroelectric for very low energies O8mm 0 15 12um 0 2uJ 1mJ 25 0000Hz 66 PE10 C Pyroelectric for low energies O12mm 0 15 12um 1uJ 10mJ 25 000Hz 66 PE10BF C As above high damage threshold O12mm 0 15 3um 10 6um 7uJ 10mJ 250Hz 66 PE25 C Medium aperture pyroelectric O24mm 0 15 3umM 8uJ 10J 10 000Hz 67 PE25BF C As above high damage threshold O24mm 0 15 3um 10 6um 60uJ 10J 250Hz 67 PE50 C Large aperture pyroelectric O46mm 0 15 3umM 10uJ 10J 10 000Hz 68 PE50BF C As above high damage threshold O46mm 0 15 3um 10 6um 120uJ 10J 250Hz 68 High energy pyroelectric sensors 10J 40J Sensor Features Aperture Spectral Range Energy Range Maximum Frequency Page PE50 DIF C Pyroelectric with diffuser high repetition rate 35MM 0 19 3um 20uJ 10J 10 000Hz 69 Complete calibration curve PE25BF DIF C Pyroelectric with diffuser for high damage 20mm 0 19 2 2uM 100 1 0J 250Hz 69 threshold Complete calibration curve PES5OBF DIF C Pyroelectric with diffuser for highest damage 035mm 0 19 2 2um 2 94um 200 uJ 10J 250Hz 70 threshold Complete calibration curve PESOBF DIFH C Similar to PESOBF DIF C but with
278. ighly compact OEM pyroelectric sensor measuring only 22 x 7 5mm with an AR coating on the surface for the wavelength of measurement It can have a simple analog output or can be supplied with a circuit board to produce calibrated analog or digital RS232 or USB output PE C RS232 OEM Sensors The new PE C Series of pyroelectric sensors has an option of RS232 output suitable for OEM use The sensors give numerical energy output and the ranges and wavelength settings can be controllable from the host PC The input and output is available at the DB9 connector at the end of the cable Ordering Information The products shown above are examples of OEM solutions developed for specific customer applications Please consult with your Ophir representative who will be happy to help you with any requirements you may have OPHIR 01 08 2013 a For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand ration Brat O OPHIR 5 Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand 2 0 Power Meters amp Interfaces Power Meter Finder The table below lists the specs and features of Ophir Power Meters and PC Interfaces Meters Vega Nova Il LaserStar LaserStar Nova StarLite Ta Dual Channel Single Channel D Digital Display Yes Yes Yes Yes Yes Yes ns Display Color Color Monochrome Monochrome Monochrome Monoch
279. ile format which are compatable in third party applications such as MatLab and Mathmatica Math program and Excel compatable ASClI csv results files Graphics in jog file format A user defined single file output that can contain settings beam displays beam profiles results in either odf or xps file formats Images reports results statistics and setup information Option to print many frames in a single operation WYSIWYG images Set Maximum Minimum limits on all calculations and statistics Red Green font color indication on result items Multiple choices for indication of failed parameters including TTL pulse for external alarm Master pass fail which triggers alarm on any failure USB signal beep stop and log alarm options Results in ASCII csv Continuous Logging Time Interval Logging Frame Count Logging Pass Fail Sampling Convert frame buffer data to third party format Export a user specified number of frames from the buffer Export Image Data ASCIl cvs Export Results ASCIl csv Export Picture jpg gif tiff bmp png file formats supported Export Image Data in Aperture PDF Operators Manual Context Sensitive Whats this Help Context Sensitive Hints Spiricon s patented Ultracal enables more accurate beam measurement and display Ultracal takes a multi frame average of the baseline offset of each individual pixel to obtain a baseline accurate to approximately 1 8 of a digital count This ba
280. indows Image Viewer se ia seman Beaipooce Teun ul A Windows viewer application enables viewing of the laser beam in a number of modes including 3D isometric plots 2D color contour plots and gray scale for thermal imaging This application enables stand alone operation of the camera independent of any other software Nevertheless the Spiricon BeamGage beam analysis software provides many additional features and capabilities not incorporated with the camera rf Nhe e Tarm e O _ vee O PT ae IOMETON ne Pyrocam IIl Windows setup menu Composite Excimer LASIK beam Composite Excimer LASIK beam profile at 193nm profile in 2D display Hybrid Integrated Circuit Sensor The Pyrocam IIl consists of a LiTaO pyroelectric crystal mounted with indium bumps to a solid state readout multiplexer This sensor developed for the Pyrocam I has proven to be the most rugged stable and precise IR detector array available Light impinging on the pyroelectric crystal is absorbed and converted to heat which creates charge on the surface The multiplexer then reads out this charge onto the video line For use with short laser pulses the firmware of the camera creates a very short electronic shutter to accurately capture the thermally generated signal 3 2 4 CERMEN Pyrocam Ill sensor array and window assembly 150 Y OPHIR Spiricon 01 08 2013 Photonics For latest updates please visit our website www
281. ing Ims 2ms 5ms 10ms 20ms we Onsen 20 msen onisma Onis 2Oims Energy Scales 10J to 10J to 10J to 10J to 10J to Ooa GU a Aoa ACK Ano 2mJ 2mJ 20mJ 20mJ 20mJ 2mJ 20m 20m 8mJ 8mJ 8mJ Lowest Measurable Energy mJ 0 2 0 4 0 8 0 8 0 8 0 1 0 1 0 2 0 5 5 5 Max Pulse Width ms 1 2 5 10 20 3 10 20 2 10 20 Maximum Pulse Rate pps 250Hz 100m SOTZ 40Hz 20Hz 40Hz 100z 5Hz 40Hz 10Hz 5Hz Noise on Lowest Range uJ 40 80 200 200 200 15 15 20 40 60 80 Additional Error with Frequency 1 1 1 2 2 1 1 1 1 1 1 Linearity with Energy for gt 7 of full scale 2 2 Damage Threshold J cm PESOBF DIFC PE50BF DIFH C Diffuser out Diffuser in lt 100ns 4 6 0 3 3 Tus 8 10 0 3 3 300us 30 30 1 10 2ms 50 50 2 20 Maximum Average Power W 9 20 30 with optional heat sink 10 15 with optional 30 40 with optional heat sink heat sink Maximum Average Power Density W cm2 200 10 500 Uniformity over surface 2 5 over central 20mm 2 over 70 of diameter 2 5 over central 20mm Weight kg 0 25 25 Version Part Number Standard Sensor 7Z02940 7Z02943 7Z02947 Previous Model Part Number 7Z02866 StarLink Sensor Direct USB link to PC p 75 787158 Calibrated at 1064nm Max additional error at other wavelengths is 2 Notes a Calibration accuracy at various wavelengths as specified here Calibrated at 1064nm 532nm and 2100nm only Specified wavelengths 193nm 248 266nm 355nm 532nm 1064nm 2100nm and 2940nm Additional
282. ing LED Indicator Thermal OEM sensor with special LED indicator where LEDs light up in proportion to power reading When power is over maximum red LEDs light up Rack Mount Laserstar Meter OEM Laserstar meter for rack mount with input from front outputs and shielded metal case on rear 2 4 1 EONS AAGE Nova OEM Board Set The Nova meter can be purchased as a board set for installation in the host system Communication with the unit is either via RS232 or via the set s own buttons output can be RS232 digital or an analog voltage Ordering Information The products shown above are examples of OEM solutions developed for specific customer applications Please consult with your Ophir representative who will be happy to help you with any requirements you may have on Q OPHIR 01 08 2013 oe For latest updates please visit our website www ophiropt com photonics MT TT ration Brat Laser Beam Analysis 111 Spiricon Photon OU OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 2 ay eee DOs R O O1 08 2013 A Newport Corporation Brand A Newport Corporation Brand A Newport Corporation Brand 3 1 EEMNES 112 01 08 2013 3 1 Choosing a Beam Profiler A laser beam profiler will increase your chance of success anytime you wish to design or apply a laser or when you find your laser system is no longer meeting specifications You would never think
283. ing screw on filter for camera with transmission of between 7 and 0 5 depending on spectral range SPZ08235 black housing Can be stacked and combined with other filters and beam splitters Two filters are included with Spiricon cameras ND3 stackable filter 4mm spacing screw on filter for camera with transmission of between 2 and 0 05 depending on spectral range Can SPZ08253 green housing be stacked and combined with other filters and beam splitters LBF 50 filter set Compact screw in filter holder with set of ND filters Attenuations from low to 106 SP90081 Filter holder and 50x50 Filter holder with set of 4 standard Schott 50X50mm neutral density filters Useful to reduce intensity before SPZ08240 filter set _ inputting into 4X beam reducer Mounts to standard 1 4 thread 2 diameter laboratory rod o Variable filter Continuously variable filter for complete control over beam intensity Especially useful for pulsed lasers Varies the SPZ17012 intensity over more than 4 orders of magnitude between wavelengths 350nm and 1100nm Can be stacked and combined with other filters and beam splitters ATP K Variable Attenuator Package provides smooth knob operated variable wedges with attenuation of optical density PH00128 ND 1 7 4 6 for a total attenuation capability of ND 7 4 Specially designed to eliminate ghost reflections fringes and light leaks Small compact module including C mount adapter to attach to camera and C mount receptac
284. instrumentation Our products are vital to medical laser manufacturers and to the hospitals and doctors who are end user laser purchasers Medical lasers cover the entire spectrum of wavelengths from the 193 nm excimer laser to the 10 6 micron CO laser where the main laser wavelengths are 193 248 532 694 755 1064 2100 2940 and 10600 nm These lasers are used for general surgery eye surgery gynecology ORL dermatology and other applications They have 3 Y Photonics A Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics 01 08 2013 01 08 2013 _ 2 OPTI outputs which start at mW and mJ on the low end going up to tens of joules and hundreds of watts at the high end The trend in medical lasers is to progress to more powerful systems especially in the dermatology field and to introduce diode lasers and intense pulsed light IPL sources instead of the traditional gas or solid state lasers Ophir has developed special equipment that can for the first time measure the output of IPL sources Regulating bodies such as the FDA in the USA require the manufacturers to have at least one channel of power or energy monitoring in each laser Ophir s high quality OEM products provide an extraordinarily efficient answer to this requirement Industrial Industrial laser customers include both laser manufacturers and laser users in job shops and factories Ophir answers the needs
285. ion InGaAs array 320x256 60dB true system dynamic range Exclusive Ultracal for ISO conforming accuracy Available with BeamGage software XEVA 100Hz 75 09 110 7 Ca USB Cameras for use with Laptop or Desktop PC se a0 Model XEVA XC 130 Description Application NIR wavelengths high resolution ROI and binning x Spectral response 900 1700nm consult factory for other options Element pitch 30um square Number or elements 320 x 256 Area 9 6 x 7 6MM Q Lens C mount Optional n Minimum system dynamic range low gain 68dB high gain 60dB LA Frame rate 100 Hz Non uniformity correction 2 Point correction plus bad pixel correction NUC files provided MM Snap shot mode Via external TTL trigger cable provided N Exposure control 1us to 400 sec in Low Gain mode Imager Cooling Thermoelectric cooler plus forced convection CY Ambient operating temperature 0 50 C Dimensions mm HxWxD 111x87x107 mm Weight camera head approx 1 8 kg Software supported BeamGage PC interface USB 2 0 special cable provided Note 1 The uncorrected rate final corrected rate will be less Q OPHIR Spiricon Photonics For latest updates please visit our website www ophiropt com photonics ay eee 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand 3 2 4 13 355nm and 1 06 3000um Pyroelectric Array Camera Pyrocam Ill Series Features m Spectral ranges
286. ion so the measurements and possibly pass fail results are completed automatic If so look for a system that has this ability Most often the capability to interface the profiler into the overall system through a LabView Excel or NET interface is available 1 2 ERRIMEN So Camera or scanning slit whichever is selected the user must first determine the laser beam measurement environment and what information about the beam profile is most important to the success of the application Ease of use and absolute spot size favors the scanning slit system while knowing about the hot and cold spots or the image of the beam under test or any low repetition pulsed laser requires a camera based beam profiling system The assistance of knowledgeable product specialists is required to provide analysis of the measurement requirements of your laser application as well as to describe the features and benefits of available products Camera based Beam Profiler Slit based Beam Profiler D OPHIR Spiricon Photon Photonics For latest updates please visit our website www ophiropt com photonics Oren Photonics OPHIR Photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand A Newport Corporation Brand 3 1 3 User Guide for Choosing the Optimum Beam Profiling System Laser Power Minimum Wavelength Beam Size lt 100mW 100mW 100W gt 100W lt 20um an gt 50um gt 500um gt 1mm NS Si NS
287. ir offers OEM sensors for any type and wavelength of laser for any power or configuration Although the power measured usually ranges from 1 150 watts the sensors can measure from tens of mW or mJ to Kilowatts or hundreds of Joules and can be cooled with water air or conduction Ophir offers a large selection of standard OEM sensors at competitive prices and excellent delivery times If required the package including the connectors can be customized to customer specifications Reliability and accuracy 1 1 5 Qxelaisveles Ophir s measuring sensors use the reliable and accurate thermopile disc principle the output is a low impedance voltage proportional to power The thermopile disc samples the entire beam making it more accurate than silicon detectors The thermopile provides a faster response than thermoelectric types Suitable absorbers which will not burn out or change reading with high power density lasers are available for any application Calibration Ophir sensors can be factory calibrated at all required wavelengths In addition to the sensors described below Ophir offers a number of other OEM sensors with larger aperture diffusers in front special absorbers single sided amplifiers voltage and ground is not required only voltage and ground and other special features Ophir also offers an OEM version of the Nova power meter consisting of just circuit boards with no casing as well as OEM sensors with RS232 or USB output inst
288. ite insensitive there This filter filters out all light below SPZ08242 1100nm to allow viewing 1300nm radiation without background interference ll Y e e e es 3 4 2 Beam Splitter Neutral Density Filters Combo Jo aa The attenuators described before can provide a high degree of attenuation however these neutral density attenuators cannot dissipate lt a more than 5W or so Therefore we often place beam splitters in front of the attenuators to reduce the intensity before the ND filters These beam splitters are made of UV grade fused silica for use from 190 to 2000nm Since they do not absorb light they have a much higher power handling capacity than the ND attenuator filters W ae N N M Model LBS 300 LBS 100 Wavelength multiple versions from 190 to 1550nm multiple versions 400 900nm 1064nm 10 6um Reflection 0 01 of incident beam 4 400 900nm 1 1064nm 0 5 or 5 10 6um Nominal ND value vis 0 3 0 7 1 2 3 4 0 3 0 7 1 2 3 4 for 300 900nm amp 1064nm 30 amp 60 for 10 6um Clear aperature O17 5mm O19mm Damage threshold see spec sheet 5W cm2 no distortion Mounting C Mount Threads Lab post mounted ue Y OPHIR Spiricon Photon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand A Newport Corporation Brand LBS 300 Beam Splitters T
289. ize Page L300W UA Large aperture built in amplifier water cooled O50mm 0 19 20uUm 0 5W 300W 80x80x58mm 53 RS232 connection L300W UAU Large aperture built in amplifier water cooled O50mm 0 19 20uUm 0 5W 300W 80x80x58mm 53 USB connection Other Sensors Ophir offers many other OEM sensors For your OEM solution please fill the questionnaire on our website 54 www ophiropt com photonics or contact us USA sales ophir spiricon com Other ophirsales ophiropt com Ta customer support ophiropt com Note a Effective Dynamic Range for a given sensor is 30 1 Ta a U BeamTrack Power Position Size Sensors A Sensor Features Aperture Spectral Range Power Range Energy Range Page 3A QUAD Power amp position very low powers up to 3W 9 5mMm 0 19 20um 100uW 3W 20 uJ 2J 56 O 3A P QUAD As above for short pulse lasers O12mm 0 15 8um 160uUW 3W 30uJ 2J 56 m 10 PPS Power position amp size to 10W O16mm 0 19 20um 20mW 10W 6uJ 2J 56 50 150 A BB 26 PPS Power position amp size to 50W 150W intermittent 26mm 0 19 20um 40mW 150W 20mJ 100J 57 F150A BB 26 PPS Power position amp size to 150W 26MM 0 19 20um 50mW 150W 20mJ 100J 57 FL250A BB 50 PPS Power position amp size to 250W large aperture O50mm 0 19 20um 150mW 250W 80mJ 300J 58 Energy sensors Photodiode and Pyroelectric Energy Sensors Photodiode energy sensors 10pJ 20pJ Sensor Features Aperture Spectral Range Energy Range Maximum Frequency Page PD10 C Very low energies down to nJ Sil
290. l focal length lenses are available to accommodate different host system focal paths The FSA includes user selectable negative lens 2 beam splitters a removable beam block on the 2nd splitter and user selectable attenuation filters prior to the beam entering the camera An excel spreadsheet is downloadable from our website that calculates which lenses are available to use for your application how far to mount the FSA from your focusing lens in order to see the focal spot and what the magnification of the image will be Operation The FSA is mounted to the camera as shown Then the assembly is placed below the final focusing lens of the laser at the recommended distance The focal spot is found by moving the assembly closer and farther from the beam until the smallest spot size is seen The exact magnification factor usually 2 3 times is calculated by moving the stage holding the FSA assembly a given lateral distance and seeing how far the centroid of the focal soot moves in the beam profiling software This scaling factor is then entered into the software In order to find focal spot shift with laser power simply find focal spot at one power change the power and measure how far the stage has to be moved up or down to get to the smallest beam size again Incoming Beam Camera Negative lens LBS 300 2nd Output Beam built in beam block Focal Spot Assembly Looking from camera mounting position 3 2 4 1 TxSelaawatarcl ais
291. l to light intensity and has a high degree of linearity over a large range of light power levels from fractions of a nanowatt to Output about 2mW Above that light level corresponding to a current of about 1mA the electron density in the photodiode becomes too great and its efficiency is reduced causing saturation and a lower reading Most Ophir PD sensors have a built in filter that reduces the light level on the detector and allows measurement up to 3W without saturation 2 Q OPHIR 01 08 2013 __ Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Power sensors 1 1 SSfelaiseyas Q OPHIR e For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation 1 1 Power Sensors Thermal Sensors As described in the general introduction the thermopile sensor has a series of bimetallic Laser junctions A temperature difference between any two junctions causes a voltage to a be formed between the two junctions Since the junctions are in series and the hot junctions are always on the inner hotter side and the cold junctions are on the outer cooler side radial heat flow on the disc causes a voltage proportional to the Hot power input Laser power impinges on the center of the thermopile sensor disc on the junction reverse side of the thermopile flows radially and is cooled on the periphery T
292. larciais 196 Y OPHIR Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand Average Laser Power RP USB 304 P RP s n 180000 ee m E With the Ophir USB Interface between the Beam Cube unit and your PC or laptop you can measure the average power of your laser to an accuracy of 3 Energy per Pulse and Frequency Energy sensor inside the Beam Cube is able to measure the energy per pulse and the frequency of the laser to high accuracy With the USB Interface you can display this on your PC or laptop screen Statistics The Beam Cube with USB Interface is able to record and store an unlimited number os Hap fr 2 iiin of points in your PC The software provided has a number of ways of displaying the Girmi AP Firei statistics of the data gii Eru a oe Fange ET ag paum z Rig i imn Tat barh ues fcth Adai as ee I Spier Hap eee al Schematic setup of a Beam Cube system ene poe m Ban k sam Ea USB2 port Pe ig if a i ans USB Interface ittilii jt es TEGi i E F Seen we a Laptop or desktop PC screen showing spatial beam profile temporal profile power energy and frequency PC scope unit optional Simplified Schematic of Beam Cube System 3 7
293. larger at 80um meaning the beams need to be at least 0 8mm to yield accurate results Scanning slit profilers can measure with better than 2 accuracy beams that are four times the slit width or larger putting the minimum beam sizes at around 8um without magnification Those investigators who want to measure their beams directly without additional optics could find this to be an advantage Power The third question is What is the power of the beam This determines the need for attenuation and or beam splitting as well as the detector type Array detectors such as silicon CCD CMOS InGaAs and Pyroelectric cameras will usually need attenuation when measuring lasers Scanning slit type profllers can measure many beams directly without any attenuation due to the natural attenuation of the slit itself Detector arrays and knife edge proflers by their nature will allow the entire beam to impact the detector at some point in the measurement leading to detector saturation unless the beam is appropriately attenuated Lasers of any wavelength with CW powers above 100mW can be measured with the pyroelectric detector equipped scanning slit profiler making it the easiest profiler for many applications Scanning slit profilers can directly measure up to kilowatts of laser power depending on the spot size or power density Y OPHIR Spiricon Photon __ Photonics For latest updates please visit our website www ophiropt com photonics 2 OPHIR Photonic
294. lation with PD300 sensors Submicrojoule and multikilohertz capability with model PE sensors All sensors use smart connector containing configuration information Program features Preferred startup configuration can be set by user User can recalibrate power or energy Response time Zero offset Ordering Information Item Description _ Ophir P N Nova Nova universal power meter for thermal pyroelectric and photodiode sensors 7Z01500 Adapter to allow Nova to operate with PE C series pyroelectric sensors Nova PE C Adapter Plugs between Nova D15 socket and PE C D15 plug 7208272 Carrying Case Carrying case 38x30x11cm For display and up to three sensors 1J02079 Nova RS232 assemblies allow Nova power meter to communicate with PC and be controlled by PC Nova RS232 Assembly RS232 adapter with standard 2 meter cable including software see page 99 78105 Nova RS232 Assembly RS232 adapter with 5 meter cable including software 781052 Nova RS232 Assembly RS232 adapter with 8 meter cable including software 781051 Battery Pack Replacement battery pack for Nova 7Z11200 Q OPHIR 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 2 1 5 StarLite Low Cost Power Energy Meter Compatible with all standard Ophir Thermal BeamTrack PE C Pyroelectric and Photodiode sensors m Brilliant large size TFT 320x240 display Compact handheld desi
295. le to easily attach additional HP series attenuators HP 266 High power laser grade fused silica reflective mirror attenuator for UV applications at 266nm Second surface anti PH00129 oe reflection coated Transmits lt 1 Useful 266 50nm HP 355 High power laser grade fused silica reflective mirror attenuator for UV applications at 355nm Second surface anti PH00130 reflection coated Transmits lt 1 Useful 355 50nm HP 450 High power laser mirror attenuator for applications in the visible from 400 500nm Second surface anti reflection PH00131 coated Transmits lt 1 Useful 450 50nm HP 600 High power laser mirror attenuator for applications in the visible from 500 700nm Transmits lt 1 PH00132 HP 800 High power laser mirror attenuator for applications in the visible Near IR from 700 900nm Transmits lt 1 PHOO133 HP 1064 High power laser mirror attenuator for applications in the Near IR from 1000 1100nm Transmits lt 1 PH00134 UV ND Filters 3 Filters holders each with 2 inconel UV ND SP90228 Filters for attunation up to ND 6 Filter for 355nm V2 givean Silicon cameras can see the 355nm 3rd harmonic radiation of YAG The YAG however usually emits some light at SPZ08246 undistorted image of the 532nm and 1064nm as well This filter filters out the other 2 wavelengths to give undistorted image of the 355nm light 355nm light Filter for 1300nm For all cameras that can operate at 1300nm but are qu
296. lections blackening begins to vaporize near this line Slits in pyro 3 0 Getctelaawatarel Nass Slit Damage Incident Power document Power density watts cm where one can begin to cut the slits Refer to Photon s Aperture Damage due to High Left Boundary Smallest beam size limited to 4 5 times the slit width Some models have another limit due to electrical bandwidth Right Boundary Instrument entrance aperture The largest beam width 1 e will be the aperture divided by 1 2 1 4 157 H Y PHIR Photon 01 08 2013 __ Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand A Newport Corporation Brand NanoScan Options and Accessories Item Description P N N52 5173 571 8 STD NS2 Si 9 5 STD NS2 Si 9 25 STD NanoScan2 Silicon Detector 3 5mm aperture 1 8micron slits High resolution head featuring Silicon detector 63 5mm diameter head with rotation mount 3 5mm entrance aperture and matched pair of 1 8micron wide slits Use from 190nm to wavelengths lt 1micron Not for 1 06micron wavelength NanoScan2 Si Detector 9mm aperture 5micron slits High resolution head featuring Si detector 63 5mm diameter head with rotation mount 9mm entrance aperture and matched pair of 5 micron wide slits Use from 190nm to wavelengths lt 1micron Not for 1 06micron wavelength NanoScan2 Si Detector 9mm aperture 25micron slits High resol
297. lectric detector 63 5mm diameter head with rotation mount 9mm entrance aperture and matched pair of 25um wide slits Use for wavelengths from 190nm to gt 20um This model does not include a cooling fan USB NS PYRO 20 25 NanoScan Large Area Pyroelectric Detector 20mm aperture 25micron slits High resolution head PH00026 featuring pyroelectric detector 100mm diameter head with rotation mount 20mm entrance aperture and matched pair of 25micron wide slits Use for wavelengths from 190nm to gt 20micron This model does not include a cooling fan USB USB NS PYRO HP 20 10 High Power NanoScan scanhead with 20mm Pyroelectric Detector 10um slits for use with higher PHO0027 power beams High resolution profiler featuring pyroelectric detector 100mm diameter scanhead with rotation mount 20 mm entrance aperture and matched pair of 10 um wide slits Can measure spots 50 um and larger 1 e diameter directly Works with CW and pulsed beams with rates greater than 2kHz Actual minimum pulse rate is dependent on beam size and scan rate USB USB NS PYRO HP 9 5 High Power NanoScan scanhead with 9mm Pyroelectric Detector 5um slits for use with higher power PH00028 beams High resolution profiler featuring pyroelectric detector 100mm diameter scanhead with rotation mount and matched pair of 5 um wide slits Use to measure spots 20um and larger 1 e2 diameter directly Works with CW and pulsed beams with rates greater than 2kHz Actual minimum pulse rate is d
298. length Range PD10 pJ C PD10 IR pJ C PE9 C PE10 C 1 3 SENLON PE50BF C PE25BF DIF C PE50 DIF C PESOBF DIF C PES0BB DIF C PE50 DIF ER C PE100BF DIF C Wavelength um Repetition Rate Range PD10 IR pJ C PE9 C PE10 C PE10BF C PE25 C PE25BF C PE50 C PE50BF C PE50 DIF C PE25BF DIF C PESOBF DIF C PE50BB DIF C PE50 DIF ER C PE100BF DIF C 01 08 2013 _ 2 A Newport Corporation Brand ort Corporatio OPHIR S ee St Ht eer eer Sa aS E 20 40 100 120 250 400 Maximum Pulse Rate Hz 1K 3K 4K 5K 10K 20K 25K For latest updates please visit our website www ophiropt com photonics n Bra 1 3 1 Photodiode Energy Sensors 10pJ to 15pJ PD10 C PD10 pJ C PD10 IR pJ C Features m Silicon and Germanium detectors Very sensitive down to 10pJ m Repetition rates to 20kHz vl Wide spectral range O N YU TA j g Model PD10 C PD10 pJ C PD10 IR pJ C Use Low energies Lowest energies Infrared Aperture mm 10 10 5 Absorber Type Si photodiode with attenuator Si photodiode Ge photodiode Spectral Range um chh 02i ae Surface Reflectivity approx 50 30 30 Calibration Accuracy 5 5 5 Energy Scales 20uJ to 20nJ 200nJ to 200pJ 20nJ to 200pJ Lowest Measurable Energy nJ 1 at 900nm 0 01 at 900nm 0 03 at 1550nm Max Pulse Width ms 0 005 0 005 0 005 Maximum Pulse Rate pps 20kHz 20kHz 10kHz Noise on Lowest Range nJ 0 05 0 001 0 01 Additional Error with Frequency a Ye COP A0 a
299. lidation tools that allows not only OSI but also the end user to verify BeamGage s basic beam width measurement algorithms It can also be used to model laser beams with special input conditions such as signal to noise background offset and bits per pixel resolution This allows the user to better understand the accuracy of measurements made under both optimum and adverse conditions This tool provides the user with a method to validate algorithms against current ISO standards and methods It can also be used to validate third party algorithms by making the output data available for use in third party applications Camera features are governed by the capabilities of the various cameras that will interface with these software products and second by which of these camera features are implimented in the software This section will describe typical camera features supported in the application Black Level Control used by Ultracal and Auto X and Auto setup Gain Control used by Auto X and Auto setup Exposure Control used by Auto X and Auto setup User Programmable ROI Pixel Binning Pixel Sampling Bits per pixel setting External Trigger Input Trigger Delay Strobe Output Strobe Delay External Trigger Probe Internal Trigger Probe These are features related to but not generally dependent upon the camera design Gamma Correction 3 2 1 4 ERRIMEN Gain Correction Bad Pixel Correction Lens
300. ll USBI and Vega devices ActiveX packages are included with the StarLab installation so as to not disrupt legacy OEM installations by customers However new features will not be added to them For new designs we highly recommend using OphirLMMeasurement Y OPHIR a For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand ort Corporatio 2 3 3 LabVIEW Solutions Ophir has long recognized the growing LabVIEW community of developers For over 10 years we have been providing LabVIEW libraries for all of our devices These are full open source applications that can be used as is or tailored by the LabVIEW programmer to his specific needs These starter applications are basic software only that allows the LabVIEW programmer to experiment freely to fully feel the strength of our devices respective command sets These applications contain VIs Virtual Instruments to control the instrument You can combine VIs to create successively larger and more versatile larger Vis by simply connecting them together Users can create sophisticated custom applications in minutes In most cases applications can be built and tested even before the instrument even arrives The versatility of these tools is limitless All of our LabVIEW libraries can be downloaded from our web site www ophiropt com VI Libraries Ophnova llb Library supplied for use with the Nova Communication is in RS232 and is based on NI VISA
301. log 1 T or T 10 ND where T is the fraction of light transmitted For example an ND of 5 lt L transmits 0 00001 or 0 001 Clear Aperture 15mm diameter Dimensions 94 W x 28 H x 43 D mm ge Thickness Tolerance 0 25mm a Mounting C mount Base Mount Y4 20 N MM Our high power laser mirror attenuator transmits lt 1 and comes in a C Mount threaded adapter ring It is also AR coated for either straight on or 45 orientation 100 HR Available standard configurations m HP 266 Use for 266 50nm m HP 355 Use for 350 50nm TATT Te FE EL erry BO 00 raU agg a20 900 950 7 90 m HP 450 Use for 450 50nm Reflectivity m HP 600 Use for 500 700nm m HP 800 Use for 700 900nm m HP 1064 Use for 1000 1100nm Other wavelengths available upon request Wavelength nm Note that if more than one reflective attenuator is required to reduce the beam power one of them must be oriented 45 to the beam Unlike absorptive attenuators reflectors cannot be stacked because they will form a laser cavity lt Q OPHIR Photon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand A Newport Corporation Brand UV ND Filters This accessory can be used with any camera fitted with C mount threads Simply thread the attenuator assembly into the front of the camera and then slide the ND filter a
302. lts m 3D displays Rotate amp Tilt All displays Pan Zoom Translate amp Z axis ZOOM 3 2 1 1 AECC Multiple beam and results windows Note quantified profile results on 3D display amp quantified 2D slices Y OPHIR Y Spiricon Photonics For latest updates please visit our website www ophiropt com photonics ee 01 08 2013 A Newport Corporation Brand A Newport Corporation Brand Newport Corporation Brand Measure Your Beam As Never Before Ultracal Essential or no big deal If you want accurate beam measurements you want Ultracal What is Ultracal Our patented baseline correction algorithm helped establish the ISO 11146 3 standard for beam measurement accuracy The problems with cameras used in beam profile measurements are a baseline or zero of the cameras drift with time temperature and b include random noise Ultracal is the only beam profiler algorithm that sets the baseline to zero and in the center of the noise Competitive products use other less sophisticated algorithms that perform a baseline subtraction but truncate the noise below the zero of the baseline This leaves only a positive component which adds a net value to all beam measurements Try the following on any other beam profiler product to see the inherent error if you don t use Ultracal 1 Measure a beam with full intensity on the profiler camera 2 Insert a ND2 filter 100X attenuation into the beam and
303. m Scan head PH00082 H I 980 VIS w lens NS lens mount bracket and 60X lens 980 WL PH00146 H I 1550 w lens NS lens mount bracket and 40X lens 1550 WL PH00081 H I High energy IR NS lens mount bracket w high energy lens WLxxx PH00147 H I 100X NS lens mount bracket and 100X lens WLxxx PH00148 Power attenuation options ND stand for Neutral Density a term used in photography to designate that a specific filter will attenuate all wavelengths across the visible equally or neutrally This is the name given to the Wratten type 96 filters which come in various Optical Densities ND1 ND2 NDO 5 etc however the proper term for beam profiling is Optical Density so the options should be OD1 OD2 etc all Item Description P N a HP ND1 350 thru 399nm Must be ordered w new system Si only PH00370 HP ND1 400 thru 700nm Must be ordered w new system Si only PH00371 ge HP ND2 400 thru 700nm Must be ordered w new system Si only PH00372 C HP ND3 400 thru 700nm Must be ordered w new system Si only PH00373 lt L HP ND1 750 thru 890nm Must be ordered w new system Si amp Ge only PH00374 HP ND2 750 thru 890nm Must be ordered w new system Si amp Ge only PHO0375 HP ND3 750 thru 890nm Must be ordered w new system Si amp Ge only PH00376 HP ND1 900 thru 1100nm Must be ordered w new system Ge only PH00377 U HP ND2 900 thru 1100nm Must be ordered w new system Ge only PH00378 aa HP ND3 900 thru 1100nm Mu
304. m 08 O12 p12 Absorber Type metallic metallic BF Spectral Range um 0 15 12 Cis 2 0 15 3 10 6 Surface Reflectivity approx 50 50 20 Calibration Accuracy 3 3 30 Max Pulse Width Setting Tus 2us 20us 1us 30us ims 5ms Energy Scales ImJ to 2uJ lim to 2uJ ImJto 20u 10mJ to 2 10mJ to 20uJ 10mJto 20W 10mJ to 200W Lowest Measurable Energy uJ 69 0 5 lt 0 2 0 5 1 1 7 a0 Max Pulse Width us 1 2 20 1 30 1000 5000 Maximum Pulse Rate pps 25kHz 15kHz 10kHz 25kHz 5kHz 250Hz 50Hz Noise on Lowest Range uJ 0 04 0 05 0 1 0 1 0 15 1 5 Additional Error with Frequency 1 to 15kHz 1 to 15kHz 1 to 10kHz 2 to 15kHz 1 to 5kHz 1 1 6 to 25kHz 3 to 25kHz Damage Threshold J cm lt 100ns 0 1 0 1 0 8 Tus 2 0 2 ie 300us 3 3 2 Linearity with Energy 1 a5 70 2 Maximum Average Power W 2 2 3 Maximum Average Power Density W cm 30 50 50 Fiber Adapters Available see page 76 ST FC SMA SC ST FC SMA SC ST FC SMA SC Weight kg 0 25 0 25 0 25 Version Part Number Standard Sensor 7Z02933 7Z02932 7Z02938 PE9 F 7Z02882 StarLink Sensor Direct USB link to PC p 75 787152 Note a Calibrated curve is checked and adjusted at 0 193 0 355 1 064 1 48 1 6 0 193 1 064 0 355 0 193 0 248 0 355 0 532 1 064 the following wavelengths um For other wavelengths in the curve there is additional 240 800nm add 4 2 3um add 8 10 6um add 15 0 2 3umM 2 10 6um 5 calibration error as stated Note b For waveleng
305. m Front Surface Attenuator Specifications Wavelength of use 200nm to 2 5um S Optical Material UV Grade Fused Silica DA Surface Quality 20 10 M Surface Accuracy A 10 Angle of Incidence 45 Clear Aperture 14mm x 14mm Reflection Polarization A nm P S Two Single Prism Front Surface Samplers 248 3 0 88 940 mounted on a ATP K Attenuator 35141 0 75 8 65 532 0 68 8 27 1064 0 64 8 01 Laser Damage Threshold CW gt 100MW crm Dimensions PFSA 38 1MM x 32 3MM x 29 5MM Dimensions DPFSA 44 5MM x 40MM x 32 5MM Output Mounting with Brass Lock Ring C Mount Male 1 32 Thread Male Input Mounting C Mount Female 1 32 Thread Female Ordering Information Model Surface P N PESA Single Prism Front Surface Sampler PH00052 DPFSA Dual Prism Front Surface Sampler PH00053 Y OPHIR Y Spiricon Photonics For latest updates please visit our website www ophiropt com photonics Sy eee ES 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport A Newport Corporation Brand Brand 3 4 4 Beam Expanders Microscope Objectives Screw on filters Model 4X Beam Expander Beam Expander with UV Converter Wavelength 193nm 360nmM 400 1800nm Object plane Beam Size Change 4X Expansion 4X OX 12X 22X 8mm in front Clear aperture 1 4 the size of the CCD of device imager Mounting C Mount Threads Camera with 4X Beam Expander Beam expanders are available for 4 5mm spacing CS mount 12 5mm spacing cameras T
306. m Monitoring 3 8 5 1 II VI CO2 Series II VI CO2 BS 35 An in line industrial laser beam monitoring solution Rapidly tune lasers for best performance for each job Monitor fluctuations while processing Optimize beams in real time Diagnose faults quickly The II VI CO BS 35 Profiler Beam Sampler was developed by II VI a leading industrial optics supplier specifically to enable measurement and viewing of high power industrial CO beams Spiricon and II VI have teamed up to provide solutions to vexing laser beam stability alignment tuning and optimizing difficulties The IIl VI CO 58 series Profiler consists of a set of turning mirrors that direct the beam to a sampling beam splitter and then returns it to the original in line path After passing through the splitter the sampled beam passes through additional attenuation and a beam telescope to size the beam for a Pyrocam Ill infrared camera The camera is connected to a PC computer through a Firewire interface A Basic Image Viewer presents 3D isometric plots 2D color contour plots and grayscale among other views Add BGS PC PIIl beam analyzer software to access many quantitative analysis Computations and charting functions The II VI CO 58 Series Profiler is similar to the BS model but the original beam is not returned in line Both a horizontal and vertical entry model are available The Pyrocam Ill with BGS PC software must be ordered separately II VI CO 58 D8 WC V
307. m UV to FIR The NanoScan s rapid beam finding and autoranging speed up the total M measurement to 20 seconds for CW lasers Both 200mm and 400mm lenses are available to generate the proper artificial waist for the laser source under test For ease of alignment there is an entrance iris on the optical axis of the NanoModeScan and a precision alignment stage for horizontal and vertical positioning NanoModeScan The ISO 11146 Method The ISO 11146 method for measuring the propagation of a laser source calls for the measurement of the beam diameter for at least 10 positions through the waist created by a test lens inserted in the beam path Five locations should be within 1 Rayleigh range of the artificial waist and at least five more points beyond two Rayleigh ranges from this waist These measurements are then used to compute the laser propagation parameters Once points are selected properly the ISO Method is the fastest measurement method and best for volume testing of lasers The Rayleigh Method The ISO method requires the user to manually select the measurement points and changing one or two of the selected points can yield different M values The Rayleigh method is completely automated selecting its own measurement points based on mapping the Rayleigh range of the beam waist This method is fully discussed in Application Note 230 Fast M k factor Measures with Photon Beam Profilers In addition the Rayleigh method can yield more
308. m beam widths plots Beam Diameter plot Mean Std Dev Min Max results displayed Power Energy Strip Charts Total Power Energy plot Peak fluence plot Avg Power plot Elliptical Results Strip Chart Elliptical orientation plot Ellipticity plot Eccentricity plot a Mean Std Dev Min Max results displayed Beam Profile Display Options Utilizes advanced hardware accelerated graphics engines All display windows can be satellited to utilize multiple display monitors Can open one each simulaneous 2D and 3D beam display windows Common color palette for 2D and 3D displays Can open X and or Y 1D beam slice profiles overlaid onto the 2D or 3D displays or in separate windows 3 2 1 4 CEMAES 128 Y OPHIR Y Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Ga Corporation Brand A Newport Corporation Brand Newport Corporation Brand Features BeamGage Standard BeamGage Professional BeamGage Enterprise all features in Standard plus all features in Pro plus Continuous software zooming in both 1D 2D and 3D displays Pan to any detector location Continuous Z axis display magnitude scaling Multiple 128 color palettes user selectable Results items can be pasted into 2D 3D 1D Pointing stability or Chart display windows Able to partition the camera imager into multiple re
309. m profile of the currently measured point in the beam propagation curve This image enables visual intuitive verification of the beam profile behavior through focus After each run the user can click any individual measured point and observe the beam profile Outlying or anomalous points can be automatically or manually excluded from the curve fit calculations for more accurate results 188 Y OPHIR Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand 3 6 1 1 Specifications for the M2 200s General Accuracy 5 typical 12 waist location and Rayleigh length typical Note Accuracy can be degraded by a variety of situations Measurement Cycle Time 2 3 minutes typical depending on setup conditions and operating mode Camera Attachment Std C mount 90 camera on axis rotation Translation System Step motor driven lead screw Translation Pitch 4 mm rev optical pitch Step Angle Sample Range 1 8 200 steps rev M 200s 190 600 mm typical Camera Specifications for GRAS20 camera Imager 1 1 8 CCD 1600 x 1200 pixels Dynamic Range 12 bit Ato D Frame Rates 7 5 FPS at full resolution Pixel size 44um x 4 4um Gain O to 25dB Shutter Control Programmable from 110us to 70ms S N Ratio 59dB at min gain Trigger Input Edge sensitive 3 3
310. m to generate a meaningful profile Please refer to Photon s Application Note Measuring Pulsed Beams with a Slit Based Profiler Q OPHIR Photon Photonics For latest updates please visit our website www ophiropt com photonics Soe One OROSA A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand New Configurable User Interface In addition to new hardware the NanoScan2 has an updated integrated software package for the Microsoft Windows Platform which allows the user to display any results windows on one screen The software can select up to 16 regions of interest to allow the simultaneous measurement of up to 16 individual beams The NanoScan 2 software comes in two versions STD and PRO The NanoScan 2 pro version of the software includes Activex automation for users who want to integrate the NanoScan into OEM systems or write their own user interface screens The NanoScan into OEM systems or write their own user interface screens File Menu Quick Access Toolbar Panel Title Bar Ribbon Bar Standard Windows Controls Ribbon Tabs sat with f i z i r i Pit 3 y 4 J bya ple 13 5 Width Al urn A GETER i Proti 13 5 Width A2 um 21 a eA Dianai Al urn xf Width BGUS Designs AZ um Centred Postion Al fum Centroid Position A2 um Peak Position Al urn Peak Postion AZ uen Peak Al fenta Peak A2 fonts Ellpticiny Peraver Total Power revit
311. n m Pointing Stability RO Power optional Total Power optional m Peak in digitizer counts m Pulsed Laser Repetition Rate Both docked and undocked windows Result ROl Value Mean Dev 13 5 Width Al um 1 63 328 564 612 0 7052 13 5 Width AJ urn 1 876 317 875 622 0 9432 Dasigma Al urm i 09062 M9700 15 D sigma A2 urn 1 42 054 B40 924 23751 Centroid Position Al pri 1 1 111 0 133 0 5022 Centro Position AZ um 1 1 730 O27 1 2221 Peak Position Al urm 1 11521 19899 S014 Peak Position A um l 4156 a732 6850 Peak Al ents i 2812438 2310 688 40486 Peak A ents 1 2687898 NAIN 5 5879 Ellipticity 1 ME DA 00023 Power 1 FH w975 00273 Total Power mW 1 202 1 203 D0002 Example of the many measurements that can be made and the precision you can expect nae i p te i La em hte i aa in im Wii Lo iim E wy uy A ua Bi TEE ENE HANI NE mE nn ae t a m i oom te Li EEI F ETR mS a A E E L L A aj u E i u ut Knowing pointing stability is a critical factor in laser performance Photon OU OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Multiple Beam Analysis Software The NanoScan software is an integrated package for Microsoft Windows operating systems it can measure from one to 16 beams in th
312. n 30W continuous Power Scales 150W 30W 3W 150W 30W 3W 150W 30W 3W Power Noise Level 5mW 3mW 3mW Maximum Average Power Density kW cm 60 at 150W 0 5 0 5 Response Time with Meter 0 95 typ s 1 7 3 8 3 8 Power Accuracy 3 3 FM Linearity with Power 1 1 5 1 5 Energy Mode Energy Range 50mJ 300 60mJ 200J 60mJ 200J Energy Scales BOON SON ae0 2005 30 3J 2007 07 Minimum Energy mJ 50 60 60 Damage Threshold J cm Pulse width Single 10 50Hz Pulse width Single 10 50Hz Pulse width lt 100ns 10 50Hz 2 Wavelength DIF IN DIF OUT lt 100ns lt 100ns 5 2 1064nm 5 2 0 5MS 20 20 0 5MsS 100 25 Sve Mil 4 2 2ms 50 50 2ms 150 AO 355nm Bs 1 Cooling convection ballistic convection ballistic convection ballistic Fiber Adapters Available see page 44 ST FC SMA SC ST FC SMA SC NA Weight kg 03 0 3 0 4 Version Part number 7Z02724 7Z02722 7Z02729 Notes a At 1064nm For shorter wavelengths derate maximum energy density to b With diffuser in sensor is only calibrated 355nm 50 of above values for 1064 532 and 355nm wavelengths 266nm 50 of above values 193nm 10 of above values 30 150 A SV 17 30 150 A HE 17 30 150 A HE DIF 17 82 _ 48 64 3 8 21 16 617 g I E RO ape E REMOVABLE ap 95 140 ADJUSTABLE 95 140 aa L 75 oL 100 l Q OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand 1
313. n performed The linearity of the photodiode detector is extremely high and errors due to this factor can be ignored as long as saturation intensity is not approached For more information on calibration accuracy please see our website at www ophiropt com calibration procedure tutorial __ Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Absorption and Damage Graphs for Thermal Sensors Absorption vs Wavelength Absorption 100 P P x PF N HE SV LP HE pen i BB LP N xg LP1 Thermal BB U Ca PF DIF SV e 70 LP1 60 PF DIF 50 0 1 1 10 100 Wavelength um Damage Threshold vs Pulse Width Note The CW power damage threshold in W cm is found on the right hand side of the table at the 1s pulse width value 100000 Energy Density in J cm SV LP1 BB thermal lt 300W 10000 LP BB thermal gt 1500W PF 1000 HE HE1 100 P 10 15 1 NS 0 3 f D 0 1 S QO o z 0 01 1E 10 1E 09 1E 08 1E 07 0 000001 0 00001 0 0001 0 001 0 01 0 1 1 Pulse Width in Seconds 2 OPHIR a For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand wport Corporation Brai 1 1 1 Photodiode Power Sensors 1 1 1 1 Standard Photodiode Sensors 50pW to 3W PD300 with filter off PD300 with filter installed
314. n the system and possibly to provide fast feedback for system control Depending on your application various configurations can be used such as m Justa sensor with raw analog output 1 3 7 Byelawseias Sensor with electronics providing an amplified or digital output Complete instrument including numeric display and or PC interface m Custom designed solution for special requirements In the following pages you will see a range of standard OEM sensors available these are actually families of existing OEM sensors with typical specifications shown They can be tailored as needed to fit your specific requirements In addition to the products described below Ophir has developed hundreds of other OEM solutions Simply contact your Ophir representative who is likely to have just the right solution to your needs 2 OPHIR a For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand rt Corporatio Standard Pyroelectric OEM Sensors Introduction Ophir manufactures three main types of pyroelectric OEM sensors Low profile pyro sensors with no electronics with a BNC output to connect to the host electronics These sensors can also be connected to an oscilloscope to measure pulse energy Since the energy of pyro sensors is proportional to the peak to valley voltage output and not the maximum voltage output the user has to take this into account in designing the electro
315. na Medicine photolithography cB Toggle Time period of soft key Go Stop measurement legends BE Average Screen NC Thermopile photodiode and pyroelectric sensors 1 i 3 LJ aes ated a D t te with PE C series of lectri ELAPSED TIME 00 06 2 TMe period oe ae operate wi sclera pyroelectric sensors ETOP RESET ESIT AAO m Periodic 1 3 sec to 30 sec or continuous 10 sec to 1 hour average for fast changing or slow changing laser Toggle Go Stop Specifications Power Meter High legibility 32 x 122 pixel graphics supertwist LCD with switchable electroluminescent backlight Large 12mm digits Features Many screen features including power with bar graph energy average exposure frequency graphs and more Outputs RS232 and analog output 1V f s optional Screen Refresh 15 times sec Case Molded high impact plastic with kickstand and EMI conductive shielding to allow use even in proximity to pulsed lasers Size Very compact 205 x 95 x 39mm Battery Rechargeable 12 volts 22 hours use between charges The charger can be ordered from your local distributor The charder also functions as AC adapter Data Handling Data can be viewed on board or transmitted to PC On Board Max data logging rate gt 10 points s Transmitted to PC Data transmission rate of 50 points s RS232 baud rate of 19200 Sensor features Works with thermopile pyroelectric and photodiode sensors Automatic continuous background cancel
316. nable ROI features BEAMSTAR TO BGP UPGRADE Upgrade any BeamStar FX or SP based product to BeamGage Professional Edition Requires a camera key SP90229 to activate SP cameras may require a firmware upgrade to enable ROI features BEAMSTAR TO BGE UPGRADE Upgrade any BeamStar FX or SP based product to BeamGage Enterprise Edition Requires a camera key to SP90230 activate SP cameras may require a firmware upgrade to enable ROI features LBA TO BGS UPGRADE Upgrade any LBA FW USB USB SP based product to BeamGage Standard Edition Requires a camera key SP90210 to activate Older Pyrocam Ill s require a Firmware Upgrade LBA TO BGP UPGRADE Upgrade any LBA FW USB USB SP based product to BeamGage Professional Edition Requires a camera SP90231 key to activate Older Pyrocam Ill s require a Firmware Upgrade LBA TO BGE UPGRADE Upgrade any LBA FW USB USB SP based product to BeamGage Enterprise Edition Requires a camera key SP90232 to activate Older Pyrocam Ill s require a Firmware Upgrade BGS TO BGP UPGRADE Upgrade BeamGage Standard Edition to Professional Edition Requires a new camera key to activate SP90233 BGS TO BGE UPGRADE Upgrade BeamGage Standard Edition to Enterprise Edition Requires a new camera key to activate SP90234 BGP TO BGE UPGRADE Upgrade BeamGage Professional Edition to Enterprise Edition Requires a new camera key to activate SP90235 PC Accessories for Cameras PCI Express FireWire 1394a b PCI Express IEEE 1394a b FireWire car
317. nce of Sensitivity on Numerical Aperture PD300 IRG 0 8 0 7 Filter out Filter in 0 6 0 5 Note 1 2 relative responce numerical aperture Graph assumes equal intensity into all angles up to maximum N A Calibration is done with SMF N A 0 13 Typical Sensitivity Curve of PD300 BB Sensors 120 110 100 90 80 70 60 50 40 30 20 10 0 1 Filter out Filter in 400 450 500 550 600 650 700 750 800 850 900 950 1000 1050 Wavelength nm relative reading relative responce relative sensitivity PD300 Angle Dependence 0 9 08 07 PD300 Filter Out 0 6 PD300 Filter In lt tr PD300 BB 0 5 t PD300 UV filter out PD300 UV filter in 0 4 0 10 20 30 40 50 60 Angle degrees PD300 CIE spectral response vs CIE curve 12 1 0 08 a CIE Ophir 04 0 2 0 300 400 500 600 700 800 Wavelength nm Relative Spectral Response of BC20 110 100 90 80 70 60 50 40 30 20 10 4 0 340 440 540 640 740 840 940 1040 1140 Wavelength nm Graph of the approximate relative spectral response of the BC20 for purpose of interpolation if the instrument is to be used at a wavelength other than the ones that are factory calibrated Photonics A Newport Corpo
318. ncluding experimental inaccuracies produced by the various measurement instruments and environmental test conditions Users can now analyze expected results and confirm if measurement algorithms will accurately measure the beam even before the experiment is constructed BeamMaker can help laser engineers technicians and researchers understand a beam s modal content by calculating results on modeled beams for a better understanding of real laser beam profiles BeamMaker is to laser beam analysis as a function generator is to an oscilloscope 3 2 1 1 BERMES BeamMaker producing a synthetically generated Hermite TEM beam and displayed in both 2D and 3D Integrated automatic Help linked into the Users Guide Touch sensitive Tool tips are available on most all controls and What s This help can provide additional details Confused about what something is or forgot how it works just go to the top right corner and touch the What s This help icon drag it and right click on the control or menu item that you want more info about and you are taken to the explanation within the BeamGage Users Guide Y OPHIR Q Spiricon Photonics For latest updates please visit our website www ophiropt com photonics oy ee 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport A Newport Corporation Brand on Brand 3 2 1 2 BeamGage Professional Professional is an upgrade version of BeamGage St
319. ncy graphs scaling special units and more Complete on line context sensitive help screens Outputs USB RS232 and user selectable 1 2 5 and 10 Volt full scale analog output Screen Refresh 15 times sec Case Molded high impact plastic with optimized angle two level kickstand Rubberized sides for easy grip and protection against damage Size Folds to a compact 208mm Lx 117mm W x 40mm H Battery Rechargeable NiMH batteries with typically 18 hours between charges The charger can be ordered from your local distributor The charger also functions as an AC adapter Data Handling Data can be viewed on board or transmitted to pc On Board Non volatile storage of up to 250 000 data points in up to 10 files Max data logging rate 4000 points s Transmitted to PC Data transmission rate of 500 points s RS232 baud rate of 38400 Sensor Features Works with Thermopile BeamTrack Pyroelectric and Photodiode sensors Automatic continuous background cancellation with PD300 sensors Submicrojoule and multikilohertz capability with pulsed energy sensors Program Features Preferred start up configuration can be set by user User can recalibrate power energy response time and zero offset Notes a The above refers to the rate of logging every single point in turbo mode Above that rate the instrument will sample points but not log every single point Ordering Information Item Description Ophir P N Vega Vega color universal power meter for thermal pyroelectric and
320. nd 0 5 beam wand sampler see damage and saturation chart SP90324 1 wand 1 beam wand sampler see damage and saturation chart SP90325 2 wand 2 beam wand sampler see damage and saturation chart SP90326 4 wand 4 beam wand sampler see damage and saturation chart SP90327 10 wand 10 beam wand sampler see damage and saturation chart SP90283 Beam Dump 5kW Beam dump for up to 5kW continuous includes mounting bracket requires continuous water flow SP90224 5000W SH Power sensor measure CO power up to 5000W water cooling needed 7Z02119 Mounting Hardware 5000W detector Mounting hardware for 5kW power sensor Required when ordering the S0OOOW SH sensor SP90212 10kW SH V2 Power sensor measure CO power up to 10 000W water cooling needed 7202645 Mounting Hardware 10 000W detector Mounting hardware for 10KW power sensor Required when ordering the 10kW SH V2 sensor SP90213 ModeCheck storage carrying case Ruggedized ModeCheck storage carrying case SP90227 Collimating 2 Lens Adapter ModeCheck Lens Adapter MLA enables a ModeCheck to recollimate a focused CO2 laser beam SP90329 MLA should be ordered with the ModeCheck so that it can be factory installed 204 Y OPHIR Y Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Ga Corporation Brand A Newport Corporation Brand Newport Corporation Brand 3 8 5 High Power In Line Industrial Bea
321. nd coatings In addition Ophir s modern facilities have in house capability for diamond turning aspheric optics and electronic equipment assembly Our laser beam profiling activities are now centered at the Spiricon facility in Logan Utah and Photon Inc facility in San Jose California USA with complete design manufacturing testing and service facilities Ophir s wide ranging activities include Production of the most complete variety of laser measurement instrumentation in existence both off the shelf and OEM Production of very high precision infrared and visible optical components lenses mirrors metallic optics spherical aspherical and diffractive windows domes and prisms HIR suitable for military FLIR and industrial CO applications Ophir a qualifed manufacturer for some of the world s leading suppliers of night vision equipment is renowned for having developed some of the highest performing and most cost effective optical systems in the world Design and production of optical assemblies Thin film optical coatings Non contact optical equipment for distance measurement and three dimensional mapping of objects developed by Optimet a company in which Ophir has a majority share These devices are based on patented technology called Conoscopic Holography Application include dentistry microelectronics robotics quality control and mechanical shops Laser Development The history of laser development
322. nd high throughput may be of no consequence if the purpose is to characterize specific optical systems that are well understood by the investigator On the other hand when a profiler needs to be used on the factory floor for quality assurance of the manufacturing process ease of use high throughput and reproducibility become paramount In this case the profiler requiring the least fiddling is generally the best fit Here there is a competition between the intuitive and the ease of use Some people find the 2 dimensional camera array to be the most intuitive because they can relate to the idea of taking a picture of the laser beam X Y scanning slits may seem less intuitive For any process that uses or works with CW or high frequency pulsed lasers the scanning slit will have the advantage of measuring the beam directly possibly even at its focus point without additional attenuation optics The dynamic range of these systems is also broad enough to measure both the focused and the unfocused beam without changing the level of attenuation Camera arrays on the other hand will require attenuation adjustment Conversely if the important aspect of the measurement is the two dimensional image of the beam or if the laser is pulsed at a low repetition rate the array will be the solution even if it means attenuation optics Also many factory applications may want to embed the beam profiler into a manufacturing cell or a piece of automat
323. ng Fiber Adapters Available see page 44 Weight kg Version Part number Standard Sensor BeamTrack Sensor Beam Position amp Size p 56 StarLink Sensor Direct USB link to PC p 42 10A 10A V1 1 65 10 H 10A 30A BB 18 L30A 10MM 10A Low power Broadband 0 19 20 16mm 20mW 10W 10W 5W 0 5W 1mW 28 0 8 3 6mJ 2J 2 200m 6 0 3 2 2 2 convection ST FC SMA SC 0 2 V1 1 7Z02637 7Z07904 787004 64 33 5 a D ADJUSTABLE 92 127 2 5 Jao Removable Part M20x1 x 4 dee l 100 75 50 150 A BB 26 OPHIR ADIT E 50 150 A BB 26 50 150 A BB 26 General purpose Broadband 0 19 20 p 26mm 40mW 150W 150W for 1 5min 100W for 2 2min 50W continuous 150W 50W 5W 2mW 12 at 150W 17 at 50W 1 5 3 1 5 20m4J 100J 100J 30J 3J 300m4 20 0 3 5 10 30 convection ST FC SMA SC 0 3 7Z02696 7Z07900 ADJUSTABLE 100 145 30A BB 18 L30A 10MM General purpose Thin profile Broadband Broadband 0 19 20 0 15 20 o 175mm p 26mm 20mW 30W 80mW 30W 8W free standing
324. ng NanoScan PRO into an automation application test lens and a NanoScan The laser beam profiler is positioned such that it measures beam size at the geometric focus of the lens From lens theory the angle of collimation is determined by the equation q D f where q is the angle of collimation Dy is the beam size measured at the focal length and f is the focal length of the lens Once the beam size is measured at the focal length of the lens simply dividing this measured beam size by the divergence angle determines the laser beam collimation angle The beam profiler remains fixed and active alignment is easily performed in real time This level of simplicity speed and functionality is simply al A not possible with techniques involving multiple beam profile a positions Divergence Collimation test fixtures based on a high quality test lens to focus your collimated or diverging beam lt L Fixtures require a complete NanoScan System preter Oo CORRA 250 Nominal 250mm focal length lens Includes an U enclosure to block stray light lajini i __ Br aa COL FXT 250 TEL Nominal 250mm focal length lens For wavelengths of Da ee So 1 use at 1310 or 1550nm with lens repositioning Includes an enclosure to block stray light y COL FXT 500 MIR For wavelengths of use at 3 5um a COL FXT C02 Zinc selenide ZnSe lens with a focal length of 190 5mm For wavelength of use at 10 6m Includes an enclosure that holds an adjustable
325. nge with a 1 5 accuracy when used in the same geometry as calibrated The power meter screen in the software shows both the total power and the individual power in each of the beams being measured The power meter option is not available with pyroelectric detectors Q OPHIR Photon Photonics For latest updates please visit our website www ophiropt com photonics reece 101 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand Optional Automation Interface The Pro model scanheads implement an Automation Server that can be used by an Automation Client written in Visual Basic for Applications VBA C C or by an application with support for ActiveX Automation such as Microsoft Excel Microsoft Word or National Instruments LabVIEW Optional Collimation Fixture A single beam size measurement using a Collimation Fixture is all that is required to determine laser beam collimation or divergence angle Real time optical alignment can then be performed to determine best collimation No special training is needed to perform these simple measurements Unlike with most measurement shortcuts high precision collimation measurements can be performed with exceedingly high resolution higher than alternative techniques All that is ENS l l l Full featured application examples are included to help your learning required for these accurate measurements of collimation is a curve when embeddi
326. ngles NA Cone Angles NA in user specified Relative Power MFD 0 5 for nominal 9mm diameter fiber NA lt 1 Aeff lt 1 90 13 26 cm 5 22 in lt 20 seconds gt 93dB InGaAs 103cB Si input power and distribution dependent 0 dBm 1mW minimum for gt 50dB dynamic range 0053357 InGaAs detector 800 1700nm Silicon available 350 800nm Windows 2000 XP Professional Activex Automation server capability Polar profile plot single or dual orthogonal scans Rectangular profile plot single or dual orthogonal scans 3D Polar view 3D Rectangular View 2D Topographic View Beam parameter Statistics Time statistics charts Relative angular power distribution Notes window for appending user comments 267 H X 305 W x 362 L MM 10 5 X 12 x 14 25 M 13 6kg 30lbs 12 7 xX 12 7 mm 0 5 x 0 5 in measurements Ordering Information 01 08 2013 Item Description PN LD8900HD Very high dynamic range Goniometric Radiometer designed to measure Mode Field Diameter MFD and PH00198 Effective Area Aeff of single mode fiber 1P Mount for fiber cartridges Interface plate that mounts to the Scan Unit Accepts all Photon Fiber Cartridges PH00201 The cartridges insert into an opening in the plate and are held in the proper meas CC Photon Fiber Clip and Clip Cartridge The Photon Fiber Clip mounts in a modified Fitel Furukawa Cleaver PH00202 The fiber is cleaved
327. nic interface see below Low profile smart sensors to be used with Ophir smart meters These PE RE type sensors have a Remote Electronics RE module to enable interface with the meter Compact pyroelectric sensors with built in amplifiers and signal conditioners which put out a voltage proportional to energy and hold this voltage for a preset period after each pulse see below Typical output from a low profile pyroelectric sensor appears as follows 1 3 7 Wyelawelas AV Ophir low profile pyroelectric sensor output for repetitively pulsing laser In the example shown above using a low profile sensor note that energy is proportional to AV and not to the voltage above the zero level Note also that the peak rapidly decays and therefore the output depends on pulse rate and duration It follows therefore that in order to measure pyroelectric pulses the voltage level must be known before the pulse and must also compensate for pulse rate or work at a low enough pulse rate for the correction to be rendered negligible When using a sensor with built in electronics typical output appears as follows AV Output from Ophir pyroelectric OEM sensor with built in signal conditioning Note that the energy is now proportional to the output voltage and since the voltage is held for a fixed time the output is much less dependent on pulse rate or duration In the above example the user does not need to perform any signal conditioning but
328. noModeScan Linear Stage 8 4kg N _ Photon Motion Controller 1 5kg VA D g9 Ajegeras Ho p i amt Crate ee a G9 a D E EE Be hat Lala TFH ca aa a Bem teine e E oe oe a Bemmi ee a HT ZETE N a fae errn fe Amt iM O map m a aa 14 aN Fi ibe A i eet rr mi mist ie misga mep Pe ey Alignment screen in ModeScan software Measurement results screen in ModeScan software Q OPHIR Photon Photonics For latest updates please visit our website www ophiropt com photonics een Pes 01 08 2013 A Newport Corporation Brand A Newport Corporation Brand Ordering Information NanoModeScan M Systems All NanoModeScan Systems include unless otherwise noted High resolution scanhead with rotation mount Two BK 7 lenses and mounts Standard are 200 and 400mm focal length a Lens coating Choices VIS Visible 430 700nm not for use with Germanium detector NIR Near IR 650 1000nm LIR Long IR 1000 1550nm not for use with Silicon detector VLIR Very long infrared gt 1550nm The two glass lenses will not be included but instead credited toward the very long wavelength IR lens or lenses that will require an optional charge for use with MSP NS Pyro 9 5 only a OPTIONAL UV If ultraviolet application the two glass lenses will not be included instead we will send one 200 mm focal length lens coated for wavelength of use Be sure to specify XXX wavelength when ordering Item Description P N NanoMode
329. noScan v2 Integrated Software package for use with NanoScan scanheads under Microsoft Windows operating systems ActiveX automation is provided in PRO models Certificate of Calibration Beam width is traceable to National Institute of Standards and Technology NIST to better than 2 NanoScan Pyroelectric detectors calibration to better than 3 Item _ Description P N USB NS Si 25 25 STD NanoScan Si Detector 25mm aperture 25micron slits High resolution head featuring Si detector 100mm PHO00390 diameter head with rotation mount 25mm entrance aperture and matched pair of 25 0micron wide slits Use from 190nm to wavelengths lt 1micron Not for 1 06micron wavelength USB USB NS Si 25 25 PRO Software includes automation feature PH00019 NanoScan Si Detector 25mm aperture 25micron slits High resolution head featuring Si detector 100mm diameter head with rotation mount 25mm entrance aperture and matched pair of 25 0micron wide slits Use from 190nm to wavelengths lt 1micron Not for 1 06micron wavelength USB USB NS Ge 12 25 STD NanoScan Ge Detector 12 5mm Aperture 25micron slits High resolution head featuring Germanium PH00395 detector 100mm diameter head with rotation mount 12 5mm entrance aperture and matched pair of 25micron wide slits USB USB NS Ge 12 25 PRO Software includes automation feature PH00024 NanoScan Ge Detector 12 5mm Aperture 25micron slits High resolution head featuring Germanium detector 100mm diameter hea
330. nt Left Boundary Smallest beam size limited to 4 5 times the slit width Some models have another limit due to electrical bandwidth Right Boundary Instrument entrance aperture The largest beam width 1 e will be the aperture divided by 1 2 1 4 O OPHIR Photon Photonics For latest updates please visit our website www ophiropt com photonics Sree OWNS UNOSU A Newport Corporation Brand A Newport Corporation Brand NanoScan Operating Space Ge 3 5mm 1 8um TOW iW 100mWw 10mW imi dBm Power Watts 100p W 10uW THW 100nW 10nW Beam Diameter at 1 e diameter in microns Germanium Detector Responsivity Detector conversion constant incident photons to a current Detector Responsivity varies with wavelength Detects between 700 1800nm Peak responsivity is 0 7 amps watt at 1550nm Detector to detector responsivity variation can be as great as 20 Power Power in the measured laser beam Assumes a round beam diameter An elliptic beam can be approximated by using the maximum width dimension and assuming all the energy is in a beam of this diameter For extremely elliptic beams ratio gt 4 1 contact the factory Beam Diameter Circular laser spot being measured by a narrow slit Clip level method Pulsed Operation Upper limit of the operating space for pulsed laser measurements Black Coating Removed detectors are not blackened Slits are blackened to reduce back ref
331. nted Ultracal calibration method and auto aperturing to exclude noise beyond the wings of the laser beam assures the user of the most accurate measurements in the industry Designed by Our Customers Spiricon has redesigned the M 200 the world s top selling beam propagation system to include customer input increased attention to durability and operational robustness for continuous use applications three shifts a day seven days a week Novice and seasoned users will appreciate these new features along with the time tested excellence that the Spiricon M 200 measurement system has provided over the years Main Screen Functions This window displays quantitative measurements of the laser parameters These include the X and Y beam widths M or K the divergence angles the Rayleigh range and other parameters shown p re HHA Loe al Pll oe p a MD Fs Ds Co ap Sbai ot mS a fede peal cnlelaanl pum f This window presents measurements of Bi eared En beam width vs position for a given run After measuring a few points the software extrapolates a curve fit The Xs and Ys represent individual measurement points The solid lines present the best fit hyperbola of the beam propagation equation to the measured points The M and other laser parameters are computed from the best fit hyperbola since it provides a smoothing of the data points 3 6 1 Ubeeiaawatatliasis ETETEN gs a ee a er i p The 2D or 3D bea
332. nted advanced calibration algorithms Extensive set of ISO quantitative measurements ISO beam width and diameter methods Enhanced window layout tools to get the most out of the desktop display area Pass fail testing available on most all measured parameters Support for USB SPxxx series cameras Supports satellite windows on multiple monitors Continuous zoom scaling in both 2D and 3D Results logging capabilities exportable to Excel Industry std data file formats HDF5 and CSV Configurable Report Generator that allows cut and paste of results images and settings from PDF and XPS file types Statistical Analysis of all measured parameters Both Drawn and Auto Aperture for isolating beam data Integrated automatic Help linked into this odf Users Guide The BeamMic series of laser beam analyzer systems are designed for entry level or basic profiling needs The beams size shape uniformity or approximation to the expected power distribution can make or break an application Accurate knowledge of these parameters is essential to the accuracy of any laser based application As laser applications push the boundaries of laser performance it is becoming more critical to understand the operating criteria BeamMic Main Display Screen Integrated Help System File Save Load ApplicationButton Tabbed Control Access _ 1 2D Beam Display Orientation 30 00 deg Tool Windows that dock inside or float out
333. ntroid X GO 2499760602 24oolbe 02 Liazille d2 Centrold Y 80 249018902 24000722402 1162580e 02 20080Ge 02 130536e 00 2ARSerO2 LIzblie 00 4177 02 4 102602 3 37 5e 02 L343e 01 LS27e 01 30250 01 598203 Miar L8672 02 95o5e 05 0 00 100 00 Max 50021 0 24902460402 25 2000e 02 5 2000e 02 JEsi SBE fe 02 3 567e 02 4 199e 02 4 198e402 27738402 3 597 02 Q OPHIR Photonics A Newport A Newport Corporation Brand Brand For latest updates please visit our website www ophiropt com photonics Min Units 1 Bbhe 2 W 9525 05 Wren 0 00 100 00 Bain Units Z2499683e 02 um Z2489787e 02 um 247000e 02 um T 246000e 07 um 1 ABie 0i um 3 885e 02 um 3885e 402 um AETR um 4 193e402 um 27 hie 02 uim 6577 03 A TA D g9 p EA q q N M Pap 2 Spiricon OPHIR Photonics 01 08 2013 A Newport Corporation Brand 3 2 1 1 CEMAES 122 01 08 2013 Multiple Charting Options You can create strip charts for stability observations on practically any of the calculations options available See next page for sample listing Charts enable tracking of short or long term stability of your laser Chk 3 Farvet Eaa Lasd Fras Apes fon loon eee Zee 2 Sd De ee ge Ga Ma td Od Tampir hipe B78 Fiai ida PS LIEG PIJET a eed e atibti 3 22530003 ETI l i 10d i AN vH lil ALE i vil t Wr me i hs thos W TEE N Anh nett ide a pte EHSL pE
334. nts IDE s such as Microsoft Visual Studio provide functions and methods for accessing the PC s com port The following is all that you need to get your RS232 applications up and running m Appendix A5 of the Starcom User Manual P N 1J06025 contains an alphabetical listing and detailed description of all commands available with the Nova Nova ll Vega and LaserStar devices 2 OPHIR Zo For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand orporatio 2 3 2 WO Valelelnelas 108 01 08 2013 m Appendix A4 of the Starcom User Manual P N 1J06025 gives an example of polling the Nova device for measurements This was written in VB6 An appropriate RS232 assembly Nova RS232 Assembly P N 78105 for use with the Nova device Nova Il Vega RS232 cable P N 7E01206 for use with the Nova ll and Vega devices included with the Nova II Vega LaserStar RS232 cable P N 1E01121 included with the LaserStar GPIB Besides RS232 the LaserStar can also communicate via GPIB IEEE 488 1 Using the SDK supplied by the vendor of your GPIB controller hardware a LaserStar IEEE cable P N 78300 and the Starcom User Manual you can integrate the LaserStar into your GPIB solution USB Ophir provides a common interface for communication and control of all of our USB speaking devices OphirLMMeasurement is a COM object that is included as part of the StarLab installation
335. o the other three questions For the near infrared from 800 to 1700nm the choices become less abundant In the lower end of this range from 800 1300nm the CCD cameras may still work but InGaAs arrays become necessary above 1300nm These are quite expensive four to five times the cost of the silicon CCDs Scanning slit systems equipped with germanium detectors are still quite reasonably priced within a few hundred dollars of their silicon equipped cousins At the mid and far infrared wavelengths the pyroelectric cameras and scanning slits sensors with pyroelectric detectors provide viable alternatives again the best approach being determined by the answers to the subsequent questions i e Diameter Distance Beam Size The second question is What beam width or spot size do you wish to measure This question can also impact the profiler type choices Arrays are limited by the size of their pixels At the current state of the art pixels are at best around 4um for silicon arrays and considerably larger 30um to 80um with InGaAs and pyroelectric cameras This means that a UV NIR beam should be larger than 50um or roughly 10 pixels in diameter to ensure that enough pixels are utilized to make an accurate measurement Beams with spot sizes smaller than 50um can be optically magnified or expanded to be measured with a camera InGaAs camera pixels are around 30um limiting the minimum measurable beam size to 300um pyroelectric array pixels are even
336. odeScan 1780 Box PH00123 FOCTUBE20 30 C Mount fine thread focus tube with 20 30mm adjustable length for focus of lenses mounted to PH00124 extension tubes FOCTUBE30 50 C Mount fine thread focus tube with 30 50mm adjustable length for focus of lenses mounted to PHO0125 extension tubes FOCTUBE50 90 C Mount fine thread focus tube with 50 90mm adjustable length for focus of lenses mounted PH00126 to extension tubes MS TUBE Kit Tube Kit for MS 1780 PH00127 Y OPHIR Photon Photonics OPHIR Photonics A Newport Corporation Brand 3 6 1 2 oSelaawatarcl ais 191 01 08 2013 3 6 2 Slit Based Beam Propagation Analyzer M NanoModeScan The NanoModeScan combines the flexibility and speed of the NanoScan with dedicated M measurement hardware and software The NanoModeScan provides an automated measurement of M using either the ISO 11146 or the Rayleigh method The ISO Method software and hardware report the ISO 11146 parameters Times diffraction limit M Beam propagation factor K Beam waist size d Beam waist location Z a Divergence 8 Rayleigh range Z By adding the capabilities of the NanoScan to the ModeScan the range of possible measurable lasers is greatly expanded and the speed of the measurements dramatically improved The NanoScan s software controlled variable scan speed allows the measurement of both CW and kHz pulsed lasers with any NanoScan scan head cov ering the entire wavelength range fro
337. oints gathered 35 7 5an S557 y ve O 254E 03 A gt B offset ranae menu Ratio Screen Two independent sensors m Measure ratio sum difference m Normalize one sensor to the other Ca D Normalize sensor Subtract background J B to reading of A W gt Data Storage and Transmission a Non volatile storage of power and energy Le ee rae ieee ia S logging data dies I Store in up to 10 files and transmit to PC eee h O PC using Starcom Windows program provided Aare A ma Save new data in file Delete data from file date in file Every energy point can be seen ae 1 Specifications Power Meter High legibility 64 x 240 pixel graphics supertwist LCD with switchable electroluminescent backlight which operates from charger or battery Large 17mm digits Screen refresh 15Hz Features Many screen features including power with bargraph energy average exposure frequency graphs and more Outputs RS232 and analog output 1V fs Screen Refresh 15 times sec Case Molded high impact plastic with swivel display and EMI conductive shielding to allow use even in proximity to pulsed lasers Size Folds to a compact 228mm W x 195mm L x 54mm H Battery Rechargeable 18 hours between charges The charger can be ordered from your local distributor The charger also functions as AC adapter Multisensor Option Two sensors can be connected and measure independently or the ration sum or difference of the two can be displa
338. om tw e Taiwan Titan Electro Optics Co 886 2 2655 2200 sales teo com tw e a Choothong _wisuth Thailand Hakuto Thailand 662 259 6244 OA a e e Thailand Filtech 66 2880 1646 info filtechenterprise com o e Turkey Mitra A S 90 212 347 4740 teknofil mitra com tr e UK Ophir Spiricon Europe 49 410 2667 1802 thomsons spiricon de e Q OPHIR Spiricon Photon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics 2 OPHIR Photonics OPHIR Photonics A Newport Corporation Brand En Corporation Brand A Newport Corporation Brand A Newport Corporation Brand See our website at www ophiropt com photonics 13 NUM PLAT REGISTRATION INC ISO 9001 2008 ANAB ANAB 5 OPHIR Photonics A Newport A Newport Corporation Brand Brand 2 Spiricon OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand Photon OPHIR Photonics A Newport Corporation Brand
339. on Benefits m All NanoScan systems are calibrated to a NIST traceable source to ensure the ultimate in accuracy m The software finds a beam in less than 0 3 seconds and displays real time updates up to 20Hz m The Z axis datum plane of the NanoScan is known to 25um making the locating of beam waist position simple and accurate Along with the ability to measure pulsed beam diameters the NanoScan accurately measures and reports the pulse frequency of the laser ensuring that the pulsed beam measurements are stable and accurate 3 0 FERMES m The sampling interval for beam measurements is adjustable to as little as 5 7nm providing the extreme accuracy required to measure very small beams m Profile averaging and rolling averages are available to improve signal to noise m NanoScan software has built in capability to control a mechanical linear stage for measurement of beam caustic m Software has a built in M2 Wizard to assist in making manual propagation ratio measurements m Time charts allow any beam result to be charted over time m Results logging to text files m Relative power meter measurements m Optional Activex Automation commands with samples of automation programs for Excel VBA LabView and Visual Basic net The minimum frequency is a function of the beam size and the scan speed This is a simple arithmetic relationship there must be a sufficient number of pulses during the time that the slits sweep through the bea
340. on systems For NanoScan users who want to extend the measurement capability of their present systems the optical and mechanical components are also available as accessories The NFP 980 with 60 1 magnification and 1um resolution specifically designed for measurement of 980nm pump lasers is also ideal for other applications in the wavelength range between 700nm 1100 nm The NFP 1550 with 40 1 magnification and 2 6um resolution is designed for use in characterizing sources in the 1300 1600nm telecommunications wavelength band Both models come with a NanoScan GE 9 5 scanhead and the magnifying objective lens which can be rigidly mounted to an optional precision XYZ translation stage which in turn is mounted to an optical rail They also include the NanoScan Control and Data Acquisition Card and NanoScan Acquisition and Analysis Software The system has all the standard Windows file saving printing Communication and ActiveX capability For visible wavelengths the NFP VIS is equipped with the NanoScan SI 9 5 scanhead and the 60 1 microscope objective AR coated for the 400 700nm wavelength range UV Wavelengths below 360nm can also be accommodated with an optional UV corrected microscope objective For higher power and longer wavelength beams the NFP Pyro is available These systems can measure spot sizes from 5um at any wavelength from 190nm to 20um This instrument configuration naturally reduces the power density incident on the instrument by one o
341. onics A Newport Corporation Brand orporatio 01 08 2013 6 Calibration Capability at Ophir Calibration is perhaps the most important of our products In order to insure the best possible calibration of your laser measuring instrumentation Ophir takes a number of extra steps not taken by other vendors As can be seen by the absorption graphs in the sensor section laser absorbers vary with wavelength so it is not enough to calibrate at 1 wavelength If the variation in absorption with wavelength is small then the sensors are calibrated at several laser wavelengths and each laser covers a range of wavelengths If the absorption variation with wavelength is considerable the sensor software is provided with an absorption correction curve that is activated by selecting the wavelength of use In addition to the above only Ophir goes one step further and checks the curve at anumber of NIST and PTB traceable wavelengths and corrects it if necessary To do this we have a complete line of calibration lasers so that we can always calibrate at or near the customer s wavelength These lasers include powers up to 400W and both CW and pulsed lasers In addition we have a number of sensors calibrated at NIST and PTB used as calibration standards Below is a list of the calibration wavelengths used at Ophir in calibrating our standard catalog sensors In addition to calibration variation with wavelength there are other possible sources of calibration err
342. onics A Newport Corporation Brand the speed the heat flows out of the same region The response time is approximately proportional to the aperture i e a 50mm aperture disc is three times as slow as an 18mm aperture disc Thermal Surface Absorbing Heads A surface absorber typically consists of an optically absorbing refractory material deposited on a heat conducting substrate of copper or aluminum When a long pulse of several hundred us or a continuous laser beam falls on such a surface absorber the light is absorbed in a very thin layer of the surface typically 0 1 1um thickness see illustration A Although the light is absorbed in a thin layer and there converted into heat the pulse is long enough so that while energy is being deposited into the surface layer heat is also flowing out into the heat conducting substrate and therefore the surface does not heat up excessively Ophir standard surface absorbers can stand up to 10 Joules cm for 2ms pulses and up to 28kW cm for low power continuous lasers Surface Absorbers for High Power Lasers and Long Pulses 1 1 BSfelaisveles The traditional surface absorbers have a much lower damage threshold at gt 1000W where they can damage at 2 3 kW cm Ophir has developed coatings that improve the damage threshold for high power lasers These coatings are denser and have higher heat conductivity than previous coatings These LP and LP1 coatings also have a much higher damage threshold
343. ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand State Of The Art Electronics The camera features a 14 bit A D converter which digitizes deep into the camera noise This enables reliable measurement and analysis of both large signals and low level signals in the wings of the laser beam Fourteen bit digitizing also enables accurate signal summing and averaging to pull weak signals out of noise This is especially useful with fiber optics at 1 3um and 1 55um and in thermal imaging The Pyrocam IIl camera electronics incorporates 2 Firewire IEEE 1394A interface ports Multiple Pyrocam Ills can be daisy chained together using the 1394 cabling New Housing amp Chopper The Pyrocam III incorporates a new compact housing measuring only 5 5 high by 5 1 wide and 2 5 deep in the direction of the beam path This allows the camera to be inserted into smaller spaces on the optical table It also makes the camera useful as a portable camera for thermal imaging and on site field service of laser systems The Pyrocam III integral focal plane chopper helps keep the camera head compact Applications Of The Pyrocam III The Pyrocam III is an ideal camera for use in scientific laboratory investigation of laser beams This includes physics chemistry and electronic system designs As an example the photos below show a research CO laser and a research N
344. or such as nonlinearity variation with position on the surface and for pyroelectric sensors pulse frequency All of these factors are carefully taken into consideration in calibration and accounted for For a complete discussion and analysis of Ophir calibration accuracy and error budget please see our website at www ophiropt com calibration procedure tutorial Special Calibration In addition to standard calibration wavelengths shown below customers can have their Ophir sensor calibrated at additional wavelengths for more accuracy Please consult your Ophir agent for special requests Wavelengths of Calibration per Sensor Type Pulsed Continuous 193 248 254 355 365 436 532 577 633 694 755 808 820 905 980 1014 1064 1310 1550 1600 2100 2940 10600 Spectral curve P P P C C RC C P C C P C C PC C PC C P P C 01 08 2013 Photodiode sensors PD300 e e e PD300 UV e e PD300 IR PD300 3W e PD300 IRG 3A IS e Thermal sensors Standard Broadband lt 1500W e Standard Broadband gt 1500W LP1 type Comet 10K Comet 1K P type PF type PF with diffuser e HE type HE with diffuser e EX type e SV type Pyroelectric sensors PD10 C PD10 pJ C amp PD10 IR pJ C PE9 C PE10 C BF type BF with diffuser Metallic standard e PE50 DIF ER C PE50 DIF C e PE100BF DIF C e OU OPHIR __ Photonics For latest updates please visit our website
345. orporation Brand LD 8900 LD 8900R System Specifications Sensor Detector Scan Radius 84mm Pinhole Size 1000um options available _ Entrance Aperture 2mm standard optional 1em Field of View 72 144 degrees Azimuthal Scans 1 2 10 20 50 100 or 200 Spatial Sampling Resolution 0 055 degrees 3241 points scan Spectral Range Silicon detector 320 1100nm InGaAs detector 800 1700nm Optional UV 190 1100nm Source Input Power for gt 400nm Mirror Damage Threshold CW 900 W cm _ Mirror Damage Threshold Pulsed TC LDs multi mode fiber w NA gt 0 5 10 s of UW to 10 s of W Single mode fiber 1uW to 1W _ For wavelengths lt 400nm Contact Factory Source Output CW or Pulsed rep rates gt 10kHZz Parameters Measured Angular Widths FWHM 5 13 5 2 user specified clip levels _Wiirietical Apertines L O 15578 2 URE a _ Angular Width Ratios FWHM 5 13 5 2 user specified clip levels Angular Position Centroid Peak Intensity or Amplitude Centroid Peak 2 user specified locations Mode Field Diameter LD 8900R only Relative Integrated Power Relative Power in user specified cone angles about an arbitrary axis Data Update Rates Single scan updates SIZ Perpendicular Scan updates 0SHZ _ 3D Profile Acquisition Time ss TimesarePC dependent 10 azimuthal scans a 20 azimuthal scans elas 50 azimuthal scans 355 100 azimuthal scans 1S 200 azimuthal scans 140s File Saving and Data Logging Program Data and Setup
346. ors as shown below PD300 F O Adapter 7208221 7Z02210 7202213 7202212 PD300 FO SMA PD300 FO ST PD300 FO FC al i 1 4 20 BSW 1 4 20 BSW 1 4 20 BSW MOUNTING THREAD MOUNTING THREAD MOUNTING THREAD 26 26 26 32 5 32 5 32 5 VIEW A VIEW A VIEW A PD300 FO SC 26 32 6 1 4 20 BSW SC CONNECTOR MOUNTING THREAD 2 OPHIR a For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Bral 1 1 4 2 Accessories for Thermal Sensors PD300R PD300 IRG 3A IS and FPS 1 Fiberoptic Adapters and Voltage Converter SC fiber adapter ST fiber adapter FC fiber adapter SMA fiber adapter N N a9 eee Y Sensor Series Fiber adapter mounting SC fiber ST fiber FC FC APC SMA fiber N bracket 1 bracket fits adapter adapter fiber adapter adapter all fiber adapters lt Thermal Sensors 3A 3A QUAD 3A P 3A P QUAD 3A FS 3A P THz not needed 10A 10A PPS 10A P not needed ga 12A 12A P not needed 30A BB 18 30A N 18 7Z08211 50 150 A BB 26 50 150 A BB 26 PPS F150A BB 26 F150A BB 26 PPS 7208210 L50 150 A BB 35 L50 150 A LP1 35 L50 150 A PF 35 7208265 7208227 Z08226 7208229 1601236 30A P 17 30 150 A SV 17 30 150 A HE 17 7Z08230 30 150 A BB 18 30 150 A LP1 18 EUS L40 150 A L40 150 A LP1 LS0 150 A 7208238 FL250A BB 35 FL250A BB 50 PPS FL250A LP1 35 7Z08265 FL400A BB 50 FL250A BB 50 7
347. oud to hold a number of patents for our creative products that clearly demonstrate our superior expertise in physics electronics optics software and mechanics Total Commitment Ophir Spiricon Photon products play an essential role in a variety of fields medical military industrial and research where accuracy reliability and robustness are vital prerequisites We affirm our unswerving commitment to remain world leaders in the research and development of laser technology instrumentation continually striving for improvement and innovation About Ophir Optronics E Ophir Power and Energy Meters Versatility for Every Application 5 Calibration Capability at Ophir 6 1 0 Sensors 7 Laser Power and Energy Sensors Table of Contents Sensor Finder Program 5 General Introduction 15 1 1 Power Sensors 17 Power Sensors Introduction 18 Absorption and Damage Graphs for Thermal Sensors 21 1 1 1 Photodiode Power Sensors 22 ARN Standard Photodiode Sensors 10pW 3W 22 Lae Round Photodiode Sensors 20pW 3W 25 MAr Special Photodiode Sensors and Integrating Spheres 50pW 3W and 20mLux 200kLux 26 1 1 2 Thermal Power Sensors 28 ELLI High Sensitivity Thermal Sensors 30uW 12W 28 22 Low Power Thermal Sensors 20mW 150W 30 Lie Low Medium Power Thermal Sensors Apertures 17mm 35mm 30mMW 150W oe 1 1 2 4 Medium Power Large Aperture Thermal Sensors Apertures 50mm 65mm 100mW 300W 34 Li Medium High Power Fan Cooled Thermal Sensors 50mW 500W 36 Lb25 High
348. peak value The Model LD 8900HDR analysis software calculates these optical fiber parameters from the far field profile the method described in the TIA EIA FOTP 191 standard for MFD requiring a minimum of 50cB for proper measurement The TIA EIA FOTP 132 standard for A requires a minimum of 50cB for proper measurements as well This wider dynamic range provides greater signal to noise detail in the tails of the far field pattern Real time data gathering and reporting of sample optical fibers or other sources is valuable for manufacturing and quality assurance evaluation Hardware and Computer The LD 8900HDR is a modular system that allows either one dimensional or three dimensional measurements The 3D module is easily exchanged with the 1D hardware and the system can be purchased with the 1D hardware the 3D hardware or both There are specially designed fiber mounting clips available for both the 1D and 3D configurations with a specially modified fiber cleaver and clip that guarantees proper fiber alignment In addition custom mounting devices are available for high dynamic range measurements of waveguides laser diodes and LEDs The controller comprises the PC microprocessor data acquisition card scan control card and LD 8900HDR acquisition and analysis software A reference calibration standard NIST traceable 1310nm OdBm LD Light Source is also available This is the measured reference at the time of original manufacture that can be u
349. phiropt com photonics a dc O 01 08 2013 A Newport Corporation Brand A Newport A Newport Corporation Brand poration Brand 3 4 2 EERME 174 01 08 2013 LBS 100 Attenuator The LBS 100 system that is not as compact as the LBS 300 above but has larger aperture and has versions for longer wavelengths The system contains the mounting frame 1 wedge beam splitter and several attenuators The exit end of the LBS 100 is standard C mount thread so all our cameras can be mounted to the frame The wedge angle is 6 5 degrees to insure that the reflection from the rear side will not enter the camera The optical elements are flat to 1 4 wave in the visible to insure no distortion of the beam LBS 100 System 4X beam reducer Camera oe ee a on Dhara g Incoming Beam LBS 100 Lib r Laer Quail Mied B LBS 100 to 4X beam reducer adaptor The LBS beam splitter attenuator system can be combined with the 4X beam reducer as shown above to attenuate and view large beams Ordering Information Item Wavelength Absorber Neutral Wedge material Max power Clear aperture Dimensions P N range material Densities or and reflection density on ND transmission filters LBS 100 400 900nm Neutral density 0 3 0 7 1 0 2 0 Fused Silica 4 in 5W cm2forno 19mm 65mmWx55mm SP90061 recommended glass 3 0 4 0 ND at wavelength range distortion 50W H x 140mm D functional to 632nm 400 900nm cm damage 2600nmM LBS 100 YAG 1
350. photonics A Newport Corporation Brand Newport Corporation Brand Item Description P N ModeScan 1780 M System with Fire Wire BeamPro MS 1780 ModeScan Model 1780 dedicated M measurement system with 12 bit FireWire IEEE 1394a CCD PHO0096 detector for single shot pulsed and CW lasers System includes ModeScan with gimbaled mount for alignment FireWire CCD camera Photon FireWire BeamPro Acquisition and Analysis Software stand alone GUI with M Analysis Active X automation interface 200mm lens coated for Visible range 400 700nm OD 2 8 glass filter for operation gt 360nm Dimensions 62mm x 140mm x 210mm For use from 250 1100nm wavelengths UV and NIR operation will require additional specifically coated optics MS 1780 Lens Kits All lens kits contain 200mm 250mm 400mm 500mm 750mm and 1m focal length coated lens with mounting hardware and MS Tube Kit MS NIR Kit Set of lenses coated for operation in NIR 700 1100nm PH00111 MS VIS Kit Set of lenses coated for operation in VIS 400 700nm PH00104 MS UV Kit Set of lenses coated for operation in UV 250 400nm PH00097 MS YAG Kit _ Set of all the available lenses for all wavelengths MS NIR VIS and UV Kits combined and MS Tube Kit PH00118 MS TUBE Kit Set of C Mount tubes to mount lenses to the MS 1780 Includes 100mm 50mm 40mm 25mm 10mm PH00127 and 50 90mm adjustable focusing tube ModeScan 1780 Accessories UV Lens Kit MS UV kit UV lenses are all fused silica plano convex and coate
351. r beam size as well as power and single shot energy The BeamTrack sensor is illustrated schematically here and works as follows the signal coming from the sensor is now divided into 4 quadrants so by measuring and comparing the output from the 4 sections we can determine the position Jst of the center of the beam to a high degree of accuracy In addition to the 4 quadrants Quad there is now a special proprietary beam size detector After processing outputs from these Beanie various detectors the user is presented with the beam position as well as beam size Note detector that the beam size is calibrated only for a Gaussian beam of gt 3mm but for other beams it will give relative size information and will indicate if the beam is changing size For more 4 Quad Total output Using Power Sensors to Measure Single Shot Energy Although Ophir thermal power sensors are used primarily to measure power they can measure single shot energy as well where they integrate the power over time flowing through the disc and thus measure energy Since the typical time it takes for the disc to heat up and cool down is several seconds these thermal sensors can only measure one pulse every several seconds at most Thus they are suitable for what is called single shot measurement Although the response time of the sensor discs is slow there is no limit to how short the pulses measured are since the measurement is of the heat flowing through the disc after the pulse 15
352. r 7 Z08201 78 ND2 stackable filter olack housing SPZ08235 172 ND3 stackable filter green housing SPZ08253 172 NH NS Ge 3 5 1 8 PRO PHO0036 166 NH NS Ge 3 5 1 8 STD PH00407 166 NH NS Ge 9 5 PRO PH00039 166 NH NS Ge 9 5 STD PH00410 166 NH NS Ge 9 25 PRO PHO0038 166 NH NS Ge 9 25 STD PH00409 166 NH NS Ge 12 25 PRO PH00040 166 NH NS Ge 12 25 STD PHO041 1 166 NH NS Si 3 5 1 8 PRO PH00031 166 NH NS Si 3 5 1 8 STD PH00402 166 NH NS Si 9 5 PRO PH00034 166 NH NS Si 9 5 STD PH00405 166 NH NS Si 9 25 PRO PHO0033 166 NH NS Si 9 25 STD PH00404 166 NH NS Si 25 25 PRO PHO0035 166 NH NS Si 25 25 STD PH00406 166 NH HP NS 9 5 PH00044 200 NH HP NS 20 10 PH00043 200 NH PYRO 9 5 PH00041 200 NH PYRO 9 5 PRO PH00041 166 NH PYRO 9 5 STD PH00412 166 NH PYRO 9 25 PH00243 200 NH PYRO 9 25 PRO PH00243 166 NH PYRO 9 25 STD PH00416 166 NH PYRO 20 25 PH00042 200 k D OPHIR Spiricon Photon Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand a Corporation Brand OPHIR Photonics A Newport Corporation Brand OPHIR Photonics A Newport Corporation Brand A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand A Newport Corporation Brand Product P N Page NH PYRO 20 25 PRO PH00042 166 NH PYRO 20 25 STD PH00413 166 NIR200 PH00112 191 NIR250 PH00113 191 NIR400 PH00114 1
353. r Accuracy 5 a Linearity with Power 2 Cooling Water Minimum Water Flow Rate at Full Power 25 liter min Water Pressure Requirements Pressure drop across sensor 0 2MPa Pressure drop across 8 meters of 2 tubing with 9 5mm ID is 0 3MPa Water Connectors Quick connector for OD 3 8 ID nylon tubing Cable Length 10 meters Weight Kg 19 Version V1 Part number 7Z02746 Notes a Calibrated for 1 07 um Notes b Water inlet temperature range 15 20 C Water temperature rate of change lt 1 C min Notes c For beam centered within 14 of beam diameter IMPROPERLY CENTERED BEAM CAN CAUSE DAMAGE TO SENSOR Maximum tilt angle 5 degrees 30K W 143 ADJUSTABLE 1 5 QUICK CONNECT FITTING FOR 1 2 NYLON TUBING w a OU OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand 1 1 2 6 High Power Water Cooled Thermal Sensors and Power Pucks 20W to 10kW Features 5000W 5000W LP 10K W m Highest powers Water cooled A Upto 10kW 45mm and 50mm apertures U N O N a Model 5000W 5000W LP 10K W di Use General purpose High power densitiesand Highest powers long pulses and power densities Absorber Type Broadband LIP Beam deflector broadband
354. r Compact built in amplifier Compact external amplifier board Absorber Type Broadband Broadband Broadband Spectral Range um 0 19 20 0 19 20 0 19 20 Aperture mm p12 12 p12 Power Mode Maximum power AW free standing AW free standing AW free standing 20W heat sinked 20W heat sinked 20W heat sinked Minimum power 10mW 20mW 10mW Power Noise Level 0 2mW 0 5mW 0 2mW Maximum Average Power Density kW cm 23 at 20W 35 at 4W 23 at 20W 35 at 4W 23 at 20W 35 at 4W Response Time 0 95 typ sec 0 8 0 8 0 8 Power Accuracy at calibrated wavelength 3 3 a Linearity with Power 1 1 1 Amplifier power supply for A UAU versions NA 5V to 18V regulated Via host USB Energy Mode Maximum Energy 10J NA NA Minimum Energy 6mJ NA NA Energy Accuracy at calibrated wavelength 5 NA NA Maximum Energy Density J cm lt 100ns 0 3 NA NA 0 5MS 2 NA NA 2MS 2 NA NA 10ms 2 NA NA Cooling conduction conduction conduction Output Ophir smart plug 4 pin Molex Mini B USB connector Dimensions 38x38x14mm 38x38x34mmM 38x38x14mm Part number 7Z02602 Consult Ophir representative Consult Ophir representative Note a With analog A version maximum power is also limited by maximum output voltage where output voltage is at most 2V less than input voltage Note b 4 pin Molex connections Voltage Voltage Analog signal out Ground Note c Calibrated at customer selected wavelength 20C SH 20C A 20C UAU FRONT VIEW SIDE VIEW REAR VIEW 4 PIN MOLE
355. r a laser beam propagating through space the equation for the divergence 9 of an unfocused beam is given by o9 M24 m1D For a pure Gaussian TEM beam M equals 1 and thus has no impact on the calculation The calculation of the minimal beam spot is then dy 4 0 Again with M equal to 1 the focused spot is diffraction limited For real beams M will be greater than 1 and thus the minimum beam waist will be larger by the M factor Characteristics of a laser beam as it passes through a focusing lens How is M measured M cannot be determined from a single beam profile measurement The ISO DIS 11146 requires that M be calculated from a series of measurements as shown in the figure above M is measured on real beams by focusing the beam with a fixed position lens of known focal length and then measuring the characteristics of the artificially created beam waist and divergence To provide an accurate calculation of M it is essential to make at least 5 measurements in the focused beam waist region and at least 5 measurements in the far field two Rayleigh ranges away from the waist area The multiple measurements ensure that the minimum beam width is found In addition the multiple measurements enable a curve fit that improves the accuracy of the calculation by minimizing measurement error at any single point An accurate calculation of M is made by using the data from the multiple beam width measurements at known
356. r input and output N A Timing Supports time stamp for each pulse resolution 10us General Number of sensors supported One sensor per unit Can combine several units with software for display of up to 8 sensors on one PC Compatible sensors Supports all standard Ophir pyroelectric thermal and photodiode sensors Power supply Powered from USB Dimensions OKSE ZANM Notes a This is the data logging rate for every single point in turbo mode Above that rate the instrument will sample points but not log every single point b Not including RP sensors PD300 CIE BC20 and PD300 BB Ordering Information Item Description Ophir P N Juno Compact module to operate one Ophir sensor from your PC USB port Comes with software Max repetition rate for every 7Z01250 pulse 10kHz Powered from PC USB port Juno USB Cable USB2 0 A MINI B 1 unit supplied with Juno 7EO1217 cable 101 OU OPHIR Phatinies For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand 2 2 2 Pulsar Multichannel and Triggered USB Interfaces Convert your laptop or desktop PC into a multichannel power energy meter From sensor to interface to PC 1 2 and 4 channel models Plug and play with most Ophir sensors Record every energy pulse at up to 25kHz a Measure missing pulses amp trigger output with external trigger Log power and energy average statistics histograms and
357. r power density can be imaged as long as the power density limit on the optical surfaces is not exceeded Notes b The Beam Cube will not resolve pulses of energy below 20mJ unless the pulse rate is high If the energy deposited in 1 50th of a second exceeds 20mJ then the unit will be able to show the pulses even though the individual energies are below 20mJ Notes c If the beam power or energy density on the entrance window exceeds specifications the window can be removed and not used assuming that the power and energy density on the first beam splitter is below the damage threshold Ordering Information 01 08 2013 Item Description Ophir P N Beam Cube 620 BeamCube system for beam profiling and power and energy Optional PC oscilloscope for measuring SP90323 pulse change for pulsed lasers Comes with 100mm lens assembly Uses SP620 beam profiling camera 50mm lens assembly Optional 50mm lens assembly for Beam Cube SPZ08255 Optional PC oscilloscope 1MHz virtual oscilloscope for Beam Cube or BA500 to turn your PC into an oscilloscope displaying the SPE10008 temporal pulse shape Uses PC or laptop USB port VU OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics Y Spiricon OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand 3 8 High Power Applications 3 8 1 High Power NanoScan Photon s Hi
358. r selected period Useful for unstable lasers eee W 3H Power range Energy Zoom Offset Help Change Zoom bar Subtract Detailed to energy graph offset help BeamTrack Power Position Size Screen Sensor type _ _4 4 PRS gazdat a and S N E Heni Track Measurement ri parameters Power measurement 2 28 7 HW vos i ____ Position and Position and size i in 2 Gi e size graph measurement y 1 0m size amp 0mm Soft Keys Power ooo Ti i 91 For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Bran Analog Power Screen 1 2 m Perfect for adjusting and maximizing laser power Ce m Large analog needle with small digital display as well 0 861 W Choice of smaller Return display with range menu laser and average headers Energy Screen PES 1751390 Henu Energy m Pulsed energy sensors single or repetitive and thermal sensors single shot only m Frequency measurement with 1 310 J pulsed energy sensors Frequency 22 00HZ Energy range 30pS Help Energy Logging Screen m Pyroelectric and thermal sensors m Continuous scroll with up to 100 points on screen Full statistics m Store data onboard and recall Laser 1064 Points Sampled 683 every pulse Minimum 0 672mJ Average 1 138 amp mJ Maximum 200mJ Std Dev 0 392mJ Present 1 602mJ Time 00 00 03 Enlarge variation pulse to pulse DEITY Res
359. r wavelengths from 190nm to gt 20um This model does not include a cooling fan lt L USB NS PYRO 20 25 STD NanoScan Large Area Pyroelectric Detector 20mm aperture 25micron slits High resolution head PH00397 C featuring pyroelectric detector 100mm diameter head with rotation mount 20mm entrance aperture and matched pair of 25micron wide slits Use for wavelengths from 190nm to gt 20micron This model 40 does not include a cooling fan USB U USB NS PYRO 20 25 PRO Software includes automation feature PH00026 GA NanoScan Large Area Pyroelectric Detector 20mm aperture 25micron slits High resolution head featuring pyroelectric detector 100mm diameter head with rotation mount 20mm entrance aperture rs and matched pair of 25micron wide slits Use for wavelengths from 190nm to gt 20micron This model M does not include a cooling fan USB NS USB NanoScan USB Controller NS USB PH00030 M NH NS Si 25 25 STD Head only NanoScan Si 25mm aperture 25um slits PH00406 NH NS Si 25 25 PRO Head only NanoScan Si 25mm aperture 25um slits PH00035 NH NS Ge 12 25 STD Head only NanoScan Ge 12mm aperture 25um slits PHO041 1 NH NS Ge 12 25 PRO Head only NanoScan Ge 12mm aperture 25um slits PH00040 NH PYRO 9 5 STD Head only NanoScan Pyro 9mm aperture 5um slits PH00412 NH PYRO 9 5 PRO Head only NanoScan Pyro 9mm aperture 5um slits PH00041 NH PYRO 9 25 STD Head only NanoScan Pyro 9mm aperture 25um slits PH00416 NH PYRO 9 25 PRO Head only NanoScan Pyro 9mm aperture 25um sli
360. rand A Newport A Newport Corporation Brand on Brand Features BeamGage Standard BeamGage Professional BeamGage Enterprise all features in Standard plus all features in Pro plus Elliptical Results a Elliptical orientation a Ellipticity a Eccentricity Distance Measurement Cursor to Crosshair Centroid to Crosshair Area Results Beam cross sectional area Divergence Focal Length method Far field two point method Far field Wide Angle method Gaussian Fit 2D whole beam fits 1D line fits Height Width X Y Centroid Goodness of fit Roughness of fit Tophat Results 2D ane Flatness Effective Area Effective Power Energy Fractional Effective Power Energy Effective Average Fluence Uniformity Plateau Uniformity Edge Steepness 1D or 2D surface inclination Other Quantitative Items Frame Averaging Frame Summing Frame Reference Subtraction Image Convolution Camera signal noise calculator Row and Column summing with results loggable Scalable Intensity Histogram exportable X or Y axial off axis image correction Beam Stability Displays and Results per ISO 11670 Pointing Stabilty of Centroid a Scatter Plot display w histogram Mean Centroid Azimuth angle of the scatter Stability M rm S Max Radius X Y centroid peak Strip chart plots Sample Time controlled Pass Fail limits Auto scaling Beam Width Diameter Strip Charts with Results X Y M
361. rared lasers especially CO The Pyrocam III replaces non electronic mode burns and acrylic blocks by providing higher definition electronic recording of data and analysis of short term fluctuations The Pyrocam Ill is superior to other electronic methods of measuring CO lasers because the entire beam can be measured in a single pulse and additional measurements made in real time This ensures that the beam did not change during the measurement Detector Damage Threshold The Pyrocam Ill sensor is capable of operation with intensities about 106 times greater than CCD cameras This makes the camera ideal for use with high power lasers as less attenuation is required Nevertheless pulsed lasers with fluence too high can evaporate the absorbing front electrode 1 101 102 103 Maximum Energy Density J cm 2 1011 1010 109 108 107 106 Pulse Width Sec Pulsed damage threshold of pyroelectric detector coating As shown the damage threshold increases with pulse width With nanosecond and longer pulses detector saturation occurs before damage With shorter pulses it helps to increase the camera amplifier gain so that electronic saturation occurs before damage The sensor can be damaged by excessive CW power which causes crystal cracking Very fe
362. ration Brand Newport Corporation Brand For latest updates please visit our website www ophiropt com photonics 1 1 1 2 Round Photodiode Sensors 20pW to 3W Features Round geometry for easy centering PD300R Filter Off PD300R Filter installed Threaded to fit standard SM1 bench equipment Same performance as standard PD300 sensors Comes with removable filter as standard Fiber optic adapters available Model PD300R PD300R 3W Use General Powers to 3W Detector Type silicon silicon Aperture o10mm o10mm Filter mode Filter out Filter in Filter out Spectral Range nm 350 1100 430 1100 350 1100 Power Range 30mW to 300mW to 100mW to 500pW 200UW 5nW Power Scales 30mW to 300mW to 100mW to 30nW and 30mW and 300nW and dBm dBm dBm Resolution nW 0 01 NA 0 1 Maximum Power vs nm mW mW nm mW Wavelength lt 488 30 300 lt 488 100 633 20 300 633 100 670 13 200 670 100 790 10 100 790 100 904 10 100 904 100 1064 25 250 1064 100 Accuracy including errors due to temp variations error vs Wavelength nm 10 360 400 NA 10 360 400 3 400 950 5 430 950 3 400 950 5 950 1100 7 950 1100 5 950 1100 Damage Threshold W cm 10 50 10 Max Pulse Energy uJ 2 20 20 Noise Level for filter out pW 20 200 Response Time with Meters 0 2 0 2 Beam Position Dependence 2 2 Fiber Adapters Available FC ST SC SMA FC ST SC SMA see page 44 Version Part Number 7Z02436 7Z02437 For graphs see page 24
363. re Results Priority Results priority will slow the capture rate to be in sync with the computational results and display updates Frame Priority Frame priority will slow results and display updating to insure that frames are collected and stored in the frame buffer as fast as possible replaces block mode a Stop After Will collect a set number of frames and then stop replaces Single Shot mode a Periodic Will collect frame at a programmed periodic rate a Periodic Burst Will collect frames in a Burst at programmed periodic rates Post processing is still available but is done via a different mechanism and is limited to only data file sources Video Playback Video playback post processing and post analysis User customizable playback rates Video file quick pan search controls Whole video file playback looping with sub selection looping Playback Video produced by logging Almost all measurements can be performed on video files System Requirements PC computer running Windows7 32 64 or XP 32 Pro Laptop or Desktop Note that some cameras require a 32bit OS Consult factory for latest 64bit camera availability 64bit OS required for Lw11058 camera Not all cameras run in all Microsoft 05 versions see camera section for specifics GHz Pentium style processor dual core recommended Minimum 2GB RAM 4GB required for Lw11058 camera Minimum 3 4GB RAM Accelerated Graphics Processor
364. re performs rigorous data analyses on the same parameters in accordance with the ISO standards providing quantitative measurement of numerous beam spatial characteristics Pass Fail limit analysis for each of these parameters can be also applied ISO Standard Beam Parameters Dslit Denergy D40 Centroid and Peak location Major and Minor axes Ellipticity Eccentricity Beam Rotation Gaussian Fit Flat top analysis Uniformity Divergence Pointing stability 3 2 RLRE For data display and visualization the user can arrange and size multiple windows as required These may contain for example live video 2D Topographic and 3D views calculated beam parameters and summary statistics in tabular form with Pass Fail limit analysis and graphical strip chart time displays with summary statistics and overlays Custom configured instrument screens with multiple views can be saved as configuration files for repeated use Data can be exported to spreadsheets math process instrumentation and statistical analysis programs and control programs by logging to files or COM ports or by sharing using LabView or ActiveX Automation Video Dual Aperture Profiles Beam Statistics 3D Profile View 2D Topographic View Time Statistics Charts Pointing Targeting Hide measurements and features not in use for user simplicity Notes Y OPHIR Q Dan a Photonics For latest updates please visit our website www ophiropt com photonics ae 01 08 2013
365. reWire ports and basic viewer software BeamGage Standard SP90091 ie To complete this order you must add an Interchangeable Window part number to accompany this system see elow 2 PY III C A Pyroelectric array detector chopped and pulsed Grade A two FireWire ports and basic viewer software SP90092 N BeamGage Standard included To complete this order you must add an Interchangeable Window part number to LN accompany this system see below PY III C B Pyroelectric array detector chopped and pulsed Grade B two FireWire ports and basic viewer software SP90093 C BeamGage Standard included To complete this order you must add an Interchangeable Window part number to lt L accompany this system see below Interchangeable Windows for Pyrocam III one included free with the purchase of a Pyrocam III Beam Profiler System PY III W BK7 1 064 Pyrocam III Window BK7 A R coated to 1064nm SP90101 PY III W 5i 1 05 2 5 Pyrocam Ill Window Silicon A R coated to 1 05 2 5um SP90102 PY III W Si 2 5 4 Pyrocam Ill Window Silicon A R coated to 2 5 4um SP90103 Y PY III W Ge 3 5 5 Pyrocam Ill Window Germanium A R coated to 3 5 5um SP90104 am PY II W Ge 10 6 Pyrocam Ill Window Germanium A R coated to 10 6um SP90105 st PY III W Ge 8 12 Pyrocam Ill Window Germanium A R coated to 8 12um SP90106 PY III W ZnSe 10 6 Pyrocam Ill Window Zinc Selenide A R coated to 10 6um SP90107 N PY III W ZnSe 2 5 Pyrocam Ill Window Zinc Selenide A R coated to 2 5um SP9
366. rements are stable and accurate m The sampling interval for beam measurements is adjustable to as little as 5 7nm providing the extreme accuracy required to measure very small beams m Profile averaging and rolling averages are available to improve signal to noise m NanoScan software has built in capability to control a mechanical linear stage for measurement of beam caustic Software has a built in M Wizard to assist in making manual propagation ratio measurements Time charts allow any beam result to be charted over time m Results logging to text files m Optional Activex Automation commands with samples of automation programs for Excel VBA LabView and Visual Basic net Optional power meter with silicon and germanium scanhead Measure Your Beam as Never Before The system has a USB 2 0 interface and operates with the latest Microsoft operating systems 64 32 bit Windows 7 and provides deep 12 bit digitization of the signal for enhanced dynamic range up to 35dB optical power The digital controller improves the accuracy and stability of the beam profile measurement by orders of magnitude It is now possible to measure beam size and beam pointing NanoScan Option NSEC with a 3 sigma precision of 1um or better The software controllable scan speed and a peak connect Side exit cable algorithm allow the measurement of pulsed and pulse width modulated lasers with frequencies of a few kHz and higher with any detector The
367. rily measured due to the pixel size of the detector array Near field profiling is performed in fiber and waveguide analysis lens characterization and other applications where beams 50 microns or smaller are analyzed While there are more accurate techniques to measure these beam sizes the camera provides two dimensional information that cannot always be obtained through knife edge or scanning slit methods This camera accessory includes base plate for mounting camera and Microscope Objective ATP K variable attenuator 50mm C Mount and an 8mm and 5mm spacer User selectable magnification lenses camera and BeamGage must be purchased separately The near field of the test beam or sample is imaged with the microscope objective lens and relayed to the camera The bracket mounting fixture holds both the lens and camera which itself can be mounting on a positioner or optical rail This complete system provides everything necessary to perform near field measurements right out of the box Camera NFP with ATP K Variable Attenuator C mount NFP Adapter Assembly ATP K Variable ND Filter 3 5 1 PERMES Fixed ND Filter Light Baffle Locking Ring 8mm C mnt extender 5mm C mnt extender Microscope Objective sold separately Ordering Information Item Description P N C NFP Assy Includes base plate for mounting camera and Microscope Objective ATP K variable attenuator SP90291 lt 50mm C Mount and an 8mm and 5mm sp
368. rmed laser industry and quickly became the leader in vibration control motion control and photonic tools Our passion is photonics our vision is to continually advance the industry by integrating leading expertise and photonics tools to create the solutions that will enable research and manufacturing to advance and create new possibilities in the markets we serve To empower this advancement Newport has become home to a comprehensive family of leading brands including New Focus with 20 years of leadership in developing manufacturing and delivering innovative high performance quality and easy to use photonics Oriel Instruments for 40 years has been a pioneer in solutions for making and measuring light Richardson Gratings for over 60 years has been the gratings leader delivering custom gratings and the largest breadth of off the shelf gratings Spectra Physics established 50 years ago was a catalyst to a new industry as the first commercial laser company and today continues to lead laser innovation And our newest addition Ophir founded in 1976 is a global leader in precision IR optics laser measurement instrumentation and 3D non contact measurement equipment Our Facilities Sited in an impressive 10 400 sq m 112 500 sq ft building in Jerusalem Israel Ophir s main manufacturing and R amp D facility is fully equipped for both the production and testing of laser measuring instrumentation optical components a
369. rome Monochrome U Analog Display Yes Yes No No No ies Rechargeable Battery Yes Yes Yes Yes Yes Yes Detector Support Thermal Sensors Yes Yes Yes Yes Yes Yes U Photodiode Sensors Yes Yes Yes Yes Yes Yes Pyroelectric Sensors Yes Yes Yes Yes Yes Yes O RP Sensors No No Yes Yes No No an BeamTrack Sensors Yes Yes No No No Yes Measurement Options O Average Power Yes Yes Yes Yes Yes Yes A Energy per Pulse Pyro Sensors Yes Yes Yes Yes Yes Yes N Single Shot Energy Thermal Sensors Yes Yes Yes Yes Yes Yes Statistics Yes Yes Yes Yes Yes No Analog Out 1V 2V 5V 10V 1V 2V 5V 10V 1V 1V 1V 1V Trigger input amp output No No No No No No Real Time Logging RS232 30Hz 30Hz 30Hz 30Hz 10Hz N A GPIB N A N A 1500Hz 1500Hz N A N A USB 2000Hz 2000Hz N A N A N A N A Bluetooth N A N A N A N A N A N A On Board Data Storage 250K 50K 50K 50K 1K No Automation Interface Yes for USB Yes for USB No No No No Labview VI s Yes Yes Yes Yes Yes No Part number 7Z01560 AO 550 7Z01601 7Z01600 7Z01500 7Z01565 Page in the catalog 89 91 93 93 2 d Ophir power meters are true plug and play instruments With all sensor information and calibration stored in the sensor plug just plug in any one of over 150 Ophir sensors and the instrument is calibrated and configured to measure laser power and energy with that sensor Position and size measurement capabilities on Vega Nova Il StarLite and Juno Power and single shot energy measurement on all instruments 01 08 2013 7 2
370. rrays to get the desired amount of attenuation This device can be used with laser outputs from microwatts to Watts Three filter holders are provided with two filters in each holder Each filter in the holder provides for a different value of attenuation To use slide the desired holder into the housing slot A click is felt when the filter is properly aligned with the beam The holders provided will allow for at tenuation of up to ND 6 C mount interface for universal application to our CCD and Pyroelectric cameras 190 380nm attenuation covers Excimer Helium Cadmium and the Nd YAG UV harmonic laser wavelengths Attenuation with these ND filters permits the best use of the dynamic range of a beam profil ing camera Attenuation range of 0 3 to 6 0 optical densities ND Set consists of three slides with two filters in each slide The Six Filters include 0 3 0 7 1 0 2 0 3 0 and 4 0 optical densities Two filters can be employed at one time for 0 3 6 0 optical attenuation in 0 3 or 0 4 ND steps 20mm clear aperture will not vignette any of our applicable camera sensors Damage threshold 100W cm for CW lasers and 20mJ cm for nano second pulse width lasers Additional Beam Splitters can be added for attenuation of high power UV lasers UV attenuation system uses high quality optics from the leader in laser beam diagnostics Fitter KD wader va Wieven LY Fangs Specifications a k EY Item UV ND Filters Nomin
371. rs D the camera 5 lt Ordering Information ge Model LBS 300 UV LBS 300 VIS LBS 300 NIR LBS 300 BB a Part No SP90183 SP90184 SP90185 SP90186 Wavelength 266 355nmM 400 700nm 1064nm 190 1550nm N Wedge Material UVFS BK7 BK7 UVFS Wedge Coating A R lt 1 AR lt 1 AR lt 1 No coating 4 reflection lt Clear aperture 17 5mm 17 5mm 17 5mm 175mm aN Reflection 0 01 0 01 0 01 0 16 Wedge ND value each ND gt 2 ND 22 ND gt 2 ND 1 3 ND Filters Inconel Bulk ND Bulk ND One each of the UV VIS amp NIR sets ND Values nominal 0 3 0 7 1 0 2 0 3 0 4 0 0 3 0 7 1 0 2 0 3 0 4 0 0 3 0 7 1 0 2 0 3 0 4 0 See UV VIS and NIR Blu holders Grn holders Red holders descriptions Filter Slides 3 5 3 9 Maximum allowable input 100 W cm CW 50 W cm 50 W cm See adjacent specifications to filter 20m4J cm2 10ns pulse 1J cm2 10ns pulse 1J cm2 10ns pulse Accessories Wedge Variable ND Filter kit N A WVF 300 SP90195 WVF 300 SP90195 WVF 300 SP90195 Beam Dumps BD 040 A 40 Watts Max Power Air Cooled SP90192 BD 500 W 500 Watts Max Power Water Cooled SP90193 Beam Deflector Assemby for 400 1100 nm only SP90263 mat C mount Wedge For additional attenuation add this to the front end of the LBS 300 Good for 350 2000nm SP90273 Splitter Note 1 ND bulk absorbing filters damage threshold is 50W cm 2 but should be used at lt 5W cm to avoid thermal lensing effects 73 Q OPHIR O Spiricon Photonics For latest updates please visit our website www o
372. s OPHIR Photonics A Newport Corporation Brand A Newport Corporation Brand A Newport Corporation Brand CW or Pulsed The final question is s the laser continuous wave CW or pulsed Lasers that operate pulsed at repetition rates less than 10 kHz are best profiled with an array Scanning apertures simply cannot make these measurements effectively in real time CW and pulsed beams with repetition rates above 10 kHz can be measured with scanning slits if the combination of the repetition rate and the beam size are sufficient to have enough laser pulses during the transit time of the slits through the beam to obtain a good profile Knife edge profilers are only able to measure CW beams Pulsed beams have other considerations when selecting a beam profiling instrument particularly pulse to pulse repeatability and pulse energy damage thresholds of the slit material or in the case of array detectors beam sampling optics 3 1 2 One More Question Besides these four questions about the physical nature of the laser to be measured there is one more that needs to be asked How accurate does the measurement need to be Not all profilers or profiler companies are equal in this regard Properly designed maintained and calibrated camera and based slit profilers can provide nanometer precision for both beam width and beam position centroid measurements A state of the art CCD array with 4um pixels can provide 2 beam width accuracy for beams larger
373. s displayed next to appropriate measurements You can also choose to perform statistical calculations on any parameter in the list fulb SS Fares Plait iina hiari aa 135 Hee 125 api 7 a z Power Energy Description ina Bal Description Value Centroid X SO 2499760e 02 um Total Pwr ISO L amp SSe 0 Centroid Y GO 2490189e 02 um Peak Loc X 150 252000e 02 um Peak Loc Y 80 248000 02 um Peak Fluence 150 3 563 05 Efficiency 50 000 in re 100 00 DicM i50 3886 07 um or Aperture El b Spatial Ddom 150 3886 02 um h DkeM 10 90 41 e 02 um Desenption ah Okem 10 90 4193e 02 um DkeM 16 84 150 4 456e 02 um Dkem 16 84 150 4 455e 02 urn DSpkMo 22650 02 wm O pkm 225le 02 um Ellipticity ggg Eccentricity ISO 1906 02 K ec Area 150 1 186 05 um Peak Loc X 150 252000 02 Peak Loc Y 50 248000e 02 DioM 150 3E6e 02 Dom 50 2bbe 02 Dao 150 3 686e 02 DkeM 10 90 41 e 02 Dkem 10 90 4 193 02 Divengence Dipk 2 767 e 02 P Gaassan Eccentricity 150 1 9e 02 Description Value Units Divergence Gauss Centroid X 2499872e 02 um Gaussian Gauss Centroid Y 2490084e 02 um TopHat Goodness of Fit 0 915 Frame Info Roughness of Fit 0 711 Small sample of possible measurements out of a list of 55 Mean Misan S 887e 02 3 bbe 02 3 88e lt 02 4 1 e 02 4 195402 2 Tisei 2 045e 02 Sample of calculation results with statistics applied Sid Dey Std Dew Ce
374. s full frame full resolution Exposure range 20uUs 27 64ms Software selectable via 1394 bus Gain 0120 B Software selectable via 1394 bus 222222 Trigger Internal or External Software selectable 22222 External Trigger Specifications 5V 1V 10mA 5mA Positive transition Trigger Connector 10 pin RJ 45 Jack Trigger Cable 10 pin RJ 45 to BNC 1 8m 0 Interface EEE 1394a FireWire 0 IEEE 1394 Cabl 1 8m Supply Voltage 8V 36V DC 12V DC nominal lt 1 ripple supplied via IEEE 1394 cable requires external powered hub with se E ES a a O Supply Power 3 5W max 12V DC typical Mechanical Filter Lens Mount C mount 1 32 tpi Mounting Gimbal Mount on 1 2 post 12mm Metric post optional Dimensions in mm 62 H x 140 W x 210 L Gimbal Mount Weight 1 4kg Environmental Operating Temperature O 50 C 32 112F Humidity 20 80 relative non condensing Conformity CE FCC ROHS and WEEE OU OPHIR Photon Ehotonie For latest updates please visit our website www ophiropt com photonics Oa Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand Arrangement of Measurement Windows Video Window Beam Propagation Mode Beam Statistics Window Horizontal and Vertical Caustics Window Ordering Information For latest updates please visit our website www ophiropt com
375. s all of the accuracy and ISO approved quantitative results that made our LBA software so successful BeamGage also brings the ease of use that has made our BeamStar software so popular Our patented UltraCal algorithm guarantees the data baseline or Zero reference point is accurate to 1 10 of a digital count on a pixel by pixel basis ISO 11146 requires that a baseline correction algorithm be used to improve the accuracy of beam width measurements UltraCal has been enhanced in BeamGage to assure that accurate spatial measurements are now more quickly available 3 2 1 1 CEMAES 118 Y OPHIR Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand See Your Beam As Never Before The Graphical User Interface GUI of BeamGage is new Dockable and floatable windows plus concealable ribbon tool bars empowers the BeamGage user to make the most of a small laptop display or a large multi monitor desktop PC foie Paw H5 ube Faak Phire H eet e aa Lo Deak y jD Gabel jii eces Daid o i bise 1 Dual or single monitor setup with beam displays on one and results on the other Note that results can be magnified large enough to see across the room PFE les Wg kga i Deis H Dam Pa ee ee igi h ee Tatal Piar 16a Geo W Peak Per 9 Se 5 Wem Beam plus resu
376. s to 10kW For high power density beams Broadband Broadband Broadband with reflective cone m beam spreader 0 2 20 1 06 and 10 6 1 06 and 10 6 o50mm o100mm os55mm 20W to 1kW 200W to 10kW 200W to 10kW 1 for same initial temperature Power 1K Model Power Damage Threshold Power Beamdia lt 40 Beam dia gt 40 100W 10 1kW 3 5 1kW 10 7 200W 8 2kW 2 8 2kW 10 6 300W 6 3kW 25 3kwW s 5 500W 5 5kW 1 5 5kW 6 3 1kW 4 10kW 10kw 4 2 5 5 5 2 1W from 20W to 1kW 2 from 1kW to 10kW 2 from 1kW to 10kW 100W 4 1kW 4 1kW 4 300W 3 3kW 3 3kW 3 400W 2 4kW 2 AkW 2 1kW 10kW 10kW 0 3 0 3 1 3 10 10 30 50 50 150 Initial reading 10s after exposure final Initial reading 20s after exposure Initial reading 30s after exposure reading 20s after exposure final reading 40s after exposure final reading 70s after exposure Temperature compensated to give accurate readings independent of starting probe temperature 70 C before measurement 140 C after measurement 2x8 character LCD Character height 5mm CE Approved AUTO Automatic measurement with laser set to 10s timed exposure Unit senses temperature rise and measures automatically MANUAL User places probe in front of beam for 10s Unit beeps to indicate start and stop measurement points History Stores last three readings Calibration Can be recalibrated by user Battery 2 x AA Lifetime in normal use approximately 1 year Weight kg 0 3 2 Te Version V1 V2 Part number 7Z02702 7Z02705 7202
377. scatter plot and stripchart results Full featured logging capabilities in a reloadable Industry standard data file format Configurable Report Generator that allows cut and paste of results images and settings NET Automation interface that allows for remote control Examples in LabView Excel and Net VB Supports English German Japanese and Chinese Windows OS in both 32 and 64bit Multilingual GUI in English Japanes and Chinese Quantitative Calculations Basic Results per ISO 11145 11146 1 3 and 13694 Power Energy Results Total power or energy Can be calibrated or sync d to an external Ophir power energy meter Peak power energy density Min Fluence Average pulse power Peak pulse power Device efficiency in Aperture Spatial Results Peak and Centroid locations Beam width Second Moment D4s Knife Edge 90 10 Knife Edge User selectable level Percent of Peak User selectable Percent of Total Energy User selectable Encircled power smallest slit 95 4 Moving slit User selectable Beam diameter a Average diameter based on x y widths Second Moment D4s a Encircled power smallest aperature 86 5 a _Encircled power smallest aperature User selectable level 3 2 1 4 RRINE Y OPHIR Y Spiricon Photonics For latest updates please visit our website www ophiropt com photonics oy ee 01 08 2013 A Newport Corporation Brand Newport Corporation B
378. sed for unit verification by the user at a later date For high dynamic range measurements in the visible spectrum a silicon detector can be substituted with a spectral range of 320 1100nm and even higher 103dB dynamic range Maximum light source unit size for direct measurements is approximately 12 7mm by 12 7mm In the 3D configuration the LD 8900HDR includes the 3D Motion Control Module and is capable of full 3D measurements with up to 200 azimuthal planes through the source 3 9 REMAIN a mee a nde a 3 3D profile of a SMF 28 optical fiber 3D polar view of LED light emission LD 8900 HDR using the LD 8900HDR O OPHIR Photon a For latest updates please visit our website www ophiropt com photonics OFFER Pones 01 08 2013 A Newport Corporation Brand ratio A Newport Corporation 3 9 ERRIMEN 210 LD 8900HDR Specifications Specifications Parameters measured Accuracy Scan range Scan radius Scan time Dynamic range Spatial sampling resolution Spectral range Software Software views Scan unit dimensions Scan unit weight Maximum light source unit size for direct 1D Single Scan Data MFD NA Aeff Single scan rectangular profile plot Fields for operator name fiber type date and user comments 3D Multi Scan Data MFD NA Aeff Angular Width Angular Centroid Angular Aspect Ratios Angular Peak Position Relative Integrated Power Relative Power in user specified cone a
379. seline offset is subtracted from each frame pixel by pixel to obtain a baseline correction accurate to 1 8 digital count Spiricon s Ultracal method retains numbers less than zero that result from noise when the baseline is subtracted Retaining fractional and negative numbers in the processed signal can increase the beam width measurement accuracy by up to 10X over conventional baseline subtraction and clip level methods Spiricon s Ultracal conforms to the best method described in ISO 11146 3 2004 Up to 256 frames can be averaged for a signal to noise ratio S N improvement of up to 16X Noise is averaged up to 1 256th 8 fractional bits Data is processed and stored in a 32bit format Up to 256 frames can be summed to pull very weak signals out of the noise Due to the precise nature of Ultracal baseline setting i e a retention of both positive and negative noise components summing of frames can be performed without generating a large offset in the baseline Choice of 5 convolution algorithms for spatial filtering for both display and calculations Spatial filtering improves the visual S N Camera features are governed by the capabilities of the various cameras that will interface with these software products and second by which of these camera features are implimented in the software This section will describe typical camera features supported in the application Black Level Control used by Ultracal and Auto X and Auto setup G
380. settings and has a wavelength range of 360 to 2500 nm Figure 1 below shows the safe average power for negligible beam distortion from thermal lensing Absorptive filters such as used in the ATP K have an upper power limit of approximately 100mW per mm beam diameter For pulsed beams Figure 2 shows the damage threshold for energy where breakage of the glass wedge may occur This is approximately 5J per mm beam diameter For lasers with power or energy levels above this the first stage of attenuation will need to come from our line of high power reflective attenuators Figure 1 Safe average 7T 685 Figure 2 Point at which pea negligible beam 00 30 ar will occur with istortion 3 500 4 35 pulsed energy amp 400 20 300 E 15 100 6 7 0129394 5 6 012934 5 6 Beam width mm Beam width mim ATP K Specifications Maximum Power Energy Handling 100 mW mm beam diameter 100 mJ total avg energy Damage threshold 5J Note Powerful laser sources may require additional attenuation prior to the beam s exposure to Model ATP K Additional attenuation usually is achieved by use of high power laser mirror attenuators or clean high quality quartz plates recommended with slight wedge angles High Power Attenuators a A Wavelength Range 360 2500 nm Near flat response out to 1500nm DN Attenuation Range Variable filters ND 1 7 to 4 6 Maximum ND 7 4 with fixed 2 8 gray glass TS attenuator C Note ND optical density
381. sfer progressive scan CCD Interline transfer progressive Interline Transfer interlaced scan CCD GED Software supported BeamGage BeamGage PC interface U B20 IEEE 1394b Host system requirements IEEE 1394 port or PCI Express or CardBus Slot Notes 1 Despite the small pixel size the spatial resolution will not exceed 50um due to diffusion of the light by the phosphor coating 2 Signal to noise ratio is degraded due to the gamma of the phosphor s response Averaging or summing of up to 256 frames improves dynamic range by up to 16x 24dB 3 In normal non shuttered camera operation the frame rate is the fastest rate at which the laser may pulse and the camera can still separate one pulse from the next With electronic shutter operation higher rate laser pulses can be split out by matching the laser repetition to the shutter speed 4 This is the damage threshold of the filter glass of the filters Assuming all filters mounted with ND1 red housing filter in the front Distortion of the beam may occur with average power densities as low as 5W cm 3 2 3 4 EEMS 2 Y OPHIR Y Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OF Photonics A Newport Corporation Brand Ga Corporation Brand A Newport Corporation Brand Newport Corporation Brand 3 2 3 5 900 1700nm InGaAs NIR Cameras Models XC 130 100Hz Features m NIR performance at room temperature High resolut
382. side App 3 2 2 RRINE j i a t i Beam Results With pm Statistics ISO Compliant Results Processing Status 3D Beam Display Indicators Buffered Video Scrolling Controls Y OPHIR Y Spiricon gt Photonics For latest updates please visit our website www ophiropt com photonics ee 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport A Newport Corporation Brand on Brand Camera Compatibility For lasers between 190 1100nm wavelenghts BeamMic interfaces to silicon CCD USB cameras For applications between 1440 1605nm BeamMic supports cost effective phosphor coated CCD cameras 190 1100nm Model SP503U SP620U Spectral Resoonse nm 190 1100nm 190 1100nm Application 1 2 format slim profile wide 1 1 8 format high resolution dynamic range CW amp pulsed wide dynamic range pulsed lasers adjustable ROI lasers CW YAG adjustable ROI Pixel spacing 9 9um X 9 9umM 440um X 4 40um Number of Elements 640 x 480 1600 x 1200 Interface Style USB USB Windows 05 support Windows 7 32 64 Vista 32 64 or XP 32 Pro May be useable for wavelengths below 350nm but sensitivity is low and detector deterioration may occur Therefore UV image converter is recommended Although our silicon cameras have shown response out to 1320nm it can cause significant blooming which could lead to errors of beam width measurement We would suggest our XC130 InGaAs cam
383. simply has to read the voltage level to determine the energy 01 2 O HIR __ Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand 1 3 7 1 Standard OEM Pyroelectric Energy Sensors 2uJ to 20mJ Features Compact Low Profle Low Cost The following specifications refer to standard OEM sensors and are to be understood as generic describing sensor families PE10 S Ophir will be happy to help you with a specific solution for your particular application Model Features Aperture mm Absorber Type Spectral Range um Surface Reflectivity approx Calibration Accuracy Sensitivity approx at 1064nm Max Pulse Width Maximum Pulse Rate pps Maximum Energy Minimum Energy Noise Equivalent Energy approx Output Damage Threshold J cm lt 100nm lus 300us Maximum Average Power W Maximum Average Power Density W cm Dimensions Part Number Notes a Notes b PE10 S High sensitivity and rep rate 12 Metallic 0 19 3 50 3 100V J into 1MQ 25S 400 20m4J 2uJ 100nJ BNC 0 1 0 2 3 2 50 50 8 x 14mm Consult Ophir representative PE10 S Q Very compact 8 Metallic 0 19 3 50 3 15V J into 1MQ and 5nF load 500us 100 20mJ 2uJ 100nJ Flying Leads 01 0 2 3 2 50 30 x 40 x 14mm Consult Ophir representative At calibrated wavelength standard 1064nm Others on request There is a trade off
384. sition Power Energy Position Size Absorber Type Broadband P type Broadband Spectral Range um OAS O 015 6 0 19 20 Aperture mm p 9 5MM p 12mm 16mm Power Mode Power Range 100UW 3W 160uUW 3W 20mW 10W Power Scales 3W to 300UW 3W to 300uW 10W 5W 0 5W Power Noise Level 5 uw 10uW 1mW Thermal Drift 30min 10 40uW 10 40 uW NA Maximum Average Power Density kW cm 1 0 05 28 Response Time with Display 0 95 typ s 1 8 De 0 8 Power Accuracy 3 3 3 Linearity with Power 1 1 1 Energy Mode Energy Range 20uJ 2J 30yJ 2J 6mJ 2J Energy Scales 2J to 200 2J to 200uJ 2J 200mJ Minimum Energy 20uJ 30uJ 6mJ Maximum Energy Density J cm lt 100ns 0 3 1 0 3 0 5ms 1 1 2 2ms 2 1 2 10ms 4 1 r Beam Tracking Mode Position Beam Position Accuracy mm Chis Os 0 1 Beam Position Resolution mm 0 02 0 02 0 02 Min Power for Position Measurement 300UW 400uUW 50mW Size Size Accuracy mm NA NA 5 50um for centered beam Size Range mm 40 beam diameter NA NA 152 0 Min Power for Size Measurement NA NA 50mW Cooling convection convection convection Weight kg 0 3 Oe Os Fiber Adapter Available see page 44 ST FC SMA SC ST FC SMA SC ST FC SMA SC Part number Standard Sensor 7Z07934 7Z07935 7Z07904 StarLink Sensor Direct USB link to PC p 42 787203 787202 Notes a The BeamtTrack features are supported by Nova Il Vega and StarLite meters Juno interface and StarLab application Notes b Depending on room airflow an
385. sor Data ASCII cvs o Export Row Column summed ASCIl cvs Export Image Data in Aperture Automation Interface NET Automation Interface with examples in LabVIEW Excel and Net VB Automate launch and termination of the application Automate start stop Ultracal Auto X and Auto Setup Automate the loading of application setups Automate control of most camera settings Automate a subset of the application features and controls Automate the capture of Binary Video Data Automate the acquisition of application results 3 2 1 4 EERME Automate the acquisition of application Images Integrated Help PDF Operators Manual Context Sensitive Whats this Help Context Sensitive Hints Signal Conditioning for Enhanced Spiricon s patented Ultracal enables more accurate Accuracy beam measurement and display Ultracal takes a multi frame average of the baseline offset of each individual pixel to obtain a baseline accurate to approximately 1 8 of a digital count This baseline offset is subtracted from each frame pixel by pixel to obtain a baseline correction accurate to 1 8 digital count Spiricon s Ultracal method retains numbers 130 Y OPHIR Y Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Ga Corporation Brand A Newport Corporation Brand vport Corporation Brand Features BeamGage Standard BeamGa
386. st be ordered w new system Ge only PH00379 HP ND1 1150 thru 1600nm Must be ordered w new system Ge only PH00380 HP ND2 1150 thru 1600nm Must be ordered w new system Ge only PH00381 aS HP ND3 1150 thru 1600nm Must be ordered w new system Ge only PH00382 M 1 2 D OPHIR Photon 01 08 2013 Photonics OPHIR Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand 3 4 1 CERME 168 01 08 2013 3 4 Accessories for Beam Profiling Introduction Spiricon has the most extensive array of accessories for beam profiling existing There are components for attenuating filtering beam splitting magnifying reducing and wavelength conversion There are components for wavelengths from the deep UV to CO wavelengths Most of the components are modular so they can be mixed and matched with each other to solve almost any beam profiling requirement needed 3 4 1 Neutral Density Attenuators Filters For almost all applications the laser beam intensity is too high for the operating range of the CCD Therefore ND glass attenuator filters are available to reduce the intensity to the proper level at the CCD In general either the LBF 50 attenuating filer set or a set of individual stackable screw on filters is recommended These filters are carefully designed not to affect beam quality or cause interference effects One stackable N
387. t Displayed beam width marker Integrated Mouse actuated pan zoom controls Manual or fixed origin placement 3D graphics utilize solid surface construction with lighting and shading effects Integrated Mouse actuated pan zoom tilt rotate controls Selectable Mesh for drawing speed vs resolution control Continuously zoomable and resizable displays in satellitable window Continuous Z axis display magnitude scaling User enabled backplanes with cursor projections Performed on all measurement functions with on screen display a Choices of intervals a Manual start stop a Time from 1 second to 1000 hours Frames from 2 to 99 999 Measurements reported Current frame data Mean Standard Deviation Minimum Maximum of each calculation performed 3 2 2 EMEARI BeamMlc Laser Beam Analyzer Software OU OPHIR at Thorn For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand P Spiricon OPHIR Photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand 3 2 2 seca Walarel ais 138 File types Printing Pass Fail Logging Exporting Integrated Help Signal Conditioning for Enhanced Accuracy Frame Averaging Frame Summing Convolution Adjacent Pixel Averaging Camera Features Camera related features in the applications Industry Standard HDF5 data and setup f
388. t Corporation Brand 143 01 08 2013 P Spiricon OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand 3 2 3 4 ERRIMEN 144 01 08 2013 3 2 3 4 1440 1605nm Phosphor Coated CCD Cameras For NIR Response Features m 1440 1605 nm Wavelengths m NIR Telecom mode field analysis m NIR Laser beam analysis Available Models m USB models SP503U 1550 SP620U 1550 m Firewire models GRAS20 1550 m Analog Camera SP 1550M GRAS20 1550 Phosphor Coating Technology The up conversion from NIR to visible light in the 1550 series cameras is nonlinear The anti Stokes phosphor coating produces visible photons at a rate roughly the square of the input signal This is shown dramatically where the camera total output increases dramatically faster than a linear output shown in the bottom line The CCD camera saturation in the center of a beam the up converted visible signal drops as the square of the input signal Thus the lower signal wings of a beam are suppressed resulting in the appearance and measurement of a beam width much smaller than actual SP 1550M SP503U 1550 SP620U 1550 1550nm Fiber Output 1610nm OPO Output This illustration is a comparison of the cross section of a beam with and without correction As seen the real width of the beam is much greater than would be observed without correction Non Linearity of SP 1550M Camera at 1550nm 4500 f Uncorrected Peak Si
389. t Corporation Brand Newport Corporation Brand 3 4 5 Beam Reducers 4X Reimaging Beam Reducer The 4X Beam Reducer is an imaging system that images the plane 30cm in front of the reducer onto the camera CCD sensor while reducing the size 4 times and inverting it The beam reducer uses the 3 screw on attenuators provided with the camera Since the intensity of a beam after reduction will be increased by 4x4 16 times it is advisable to attenuate the beam more than you would without beam reduction This can be done with additional external beam splitters and attenuators which are available see ordering information Note that the custom designed beam reducer gives better image quality than tapered fibers since it does not introduce graininess or uneven pixel response Also the image distortion of 1 is considerably lower than with most tapered fibers The beam reducer is not compatible with CS mount cameras cowl i gl Pel bis elie i TH 1 Wiss T api E Paaie Gap 1 Fadia Daph Ha aha l j i Dap 4X beam reducer A NN Shown is an image of an Alexandrite laser with beam diameter of a 18mm As can be seen it is easily seen with the FX50 camera with O the 4X beam reducer LBS 100 combined with 4X E beam reducer lt L The 4X beam reducer can be combined with the LBS 100 beam splitter attenuator system to attenuate higher power beams before reducing them in size aa Specifications of 4X beam reducer LA Spectral Range 39
390. t in pre trigger allows synchronization to even sub nanosecond pulses 2 Same connector can provide trigger out to synch laser Supports programmable delay on Strobe Out 3 Same connector accepts photodiode trigger see below Optional photodiode trigger available P N SPZ17005 1 3uUW cm 2 2UW cm 0 5nW cm 2 2UW cm 2 5nW cm 50W cm 0 1J crm with all filters installed for lt 100ns pulse width 96mm x 76MM x 16MM CCD recess 4 5mm below surface Pulsed with trigger sync excellent Pulsed with video trigger good CW poor Interline transfer progressive scan CCD 96mm x 76MM x 23mm CCD recess 4 5mm below surface Pulsed with trigger sync excellent Pulsed with video trigger good CW good dia beams CW amp pulsed lasers ideal for CW YAG Adjustable ROI 190 1100nm amp 35mm x 24mm 9 0um x 9 0umM 4008 x 2672 59 dB 1 3 1 fps at full resolution higher rates with binning and smaller region of interest 10us to multiple frame times Supports both Trigger In and Strobe Out N A 0 15 uW cm 0 17NW cm 0 15mW cm 83mm x 76mm x 128mm CCD recess 18 8mm below bezel 31 75 from ND filter holder Pulsed with trigger sync excellent Pulsed with video trigger good CW good Software supported BeamGage PC interface USR 20 TA Notes 1 Camera set to full resolution at maximum frame rate and exposure times running CW at 632 8nm wavelength Camera set to Ta minimum
391. t performance from our smart sensors As for ease of use only Ophir power meters have smart keys to give the easiest and most convenient user interface The units also come with a versatile range of software to use seamlessly either with the Ophir software or the user s own Photodiode Sensors Thermal Sensors Pyroelectric Sensors Powers pW to Watts Powers mW to kW and Energies pJ to Joules single shot energy Rep rates to 25kHz Power Meters Computer Interfaces with USB RS232 with USB Bluetooth 2 0 EOV AMVK Nova Il Juno Pulsar Vega 1 2 4 channels color general compact a h C Nova Laserstar USB Interface Quasar compact 2 channel basic wireless Software Solutions StarLab LabVIEW Starcom Activex amp COM Object Interfaces LabVIEW StarLab software 01 08 2013 _ 2 OPTI a For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand orporatio 2 1 Power Meters 2 1 1 Vega Color Screen Laser Power Energy Meter Compatible with all Ophir thermal BeamTrack pyroelectric and photodiode sensors Brilliant color large size TFT 320x240 display Compact handheld design with rubberized bumpers and optimized 2 position kickstand Choice of digital or analog needle display Illuminated keys for working in the dark Analog output Log every point at up to 4000HZz with pyro sensors Non volatile data storage up to 250 000 points
392. ted 1550nm sensor Comes with USB cable and 3 ND filters BGP USB SP620 BeamGage Professional Edition software software license 1 1 8 format 1600x1200 pixel camera with SP90238 4 5mm CCD recess Comes with USB cable and 3 ND filters BGP USB SP620 1550 BeamGage Professional Edition software software license 1 1 8 format 1600x1200 pixel camera with SP90239 45mm CCD recess Phosphor coated 1550nm sensor Comes with USB cable and 3 ND filters BGP USB L11059 BeamGage Professional Edition software software license 35mm format 4008x2672 pixel camera Comes SP90320 with universal power supply USB cable and 3 ND filters BGP USB XC1 30 BeamGage Professional Edition software software license 320x256 pixel InGaAs camera with C mount SP90241 recess 9 to 1 7um spectral band Comes with universal power supply USB cable external trigger cable and 3 ND filters consult factory for other camera options N BeamGage Professional FireWire Beam Ta Profiler Systems camera and software BGP FWB GRAS20 DESKTOP BeamGage Professional Edition software software license 1 1 8 format 1600x1200 pixel camera with SP90242D eae 12 5mm C mount CCD recess Comes with 1394b and trigger cables PCI Express interface card and 3 ND filters Desktop model BGP FWB GRAS20 LAPTOP BeamGage Professional Edition software software license 1 1 8 format 1600x1200 pixel camera with SP90242L T 12 5mm C mount CCD recess Comes with 1394b and trig
393. ted with home versions of Windows Both 64 bit and 32 bit versions of Windows 7 are supported NanoScan v2 is no longer tested on Windows XP 32 bit operating systems 2 The computer memory RAM will affect the performance of the software in the Data Recorder 157 E VU OPHIR Photon Photonics For latest updates please visit our website www ophiropt com photonics en Pes 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand Specifications Model Bus interface Signal digitization Maximum digitization clock Maximum update rate Data transfer On board memory Weight Operating temperature Humidity Scanhead Dimensions Power CPU Clock Memory Clock Scanning Motor YAG Focal Spot Analyzer USB 2 0 16bit 2OMHz 20Hz Bulk Transfer Mode 64MB mDDR SDRAM 434g 15 3 ounces 0 50 C 90 non condensing 3 85 9 78cm L X 2 5 6 35cm USB 2 0 Bus Powered 300MHz 264MHz Brushed DC 4W max Mechanical Dimensions NanoScan2 Standard Scanhead NS2 Si and NS2 Ge 0 7440 025 f Reference Surface Measurement Plane N 0 38 0 05 m DETAIL A Y SCALE Scan Head Rotation D Adjustment Screw 2 m 38 1 T 1 32 Thread Reference Surface C Mount A i 55 3 ge YU aa 063 4 M p 40 4 681 8 o M Mounting Hole ocation Reference 7 1 4 20 Mountin
394. ter Flow Rate at Full Power N A 4 5 liter min 9 liter min Weight kg 0 9 2 8 4 5 Version Part number 7Z17200 7Z17201 7Z17202 Notes a Water temperature range 18 30 C Water temperature rate of change lt 1 C min Notes b Max power and energy density Beam diameter Max power density Max energy density 1ms pulse width 3ms pulse width 10ms pulse width lt 15mm 10kW cm 30J cm 60J cm 150J cm 15 20mm 7kW cm 20J cm 40J cm 100J cm 20 40mm 5kW cm 15J cm 30J cm 70J cm 40 45MM AkW cm 12J cm 25J cm 60J cm BD5000W BB 50 BDFL500A BB 50 P 105 90 7 j 0146 72 50 2x 1 8 NPT THREAD SIZE J145 l Tas S 27 f FT ADJUSTABLE i T ADJUSTABLE 2x M3 x 4 5 dee 135 180 ra E 16 5 DEPOWEK 107 153 id 2x QUICK CONNECT FITTING upply socket oo FOR 3 8 PLASTIC HOSE i wee 75 Po es a 146 18 5 ADJUSTABLE 4 8 NET 135 180 THREAD SIZE FOR 0578 PLASTIC HOSE 100 Q OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand 1 1 5 OEM Solutions Introduction Many laser systems manufacturers need to have a measuring capability built into their systems Ophir is the world s leading supplier of OEM laser power energy measurement instrumentation which can be built into host systems such as medical industrial etc With extensive experience accumulated in the field Ophir offers the largest variety of OEM products and is therefor
395. test updates please visit our website www ophiropt com photonics seer Ones O08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand 3 0 eteelaaavarclNasiis 157 D 01 08 2013 The Most Versatile and Flexible Beam Profiling System Available Photon s NanoScan scanning slit profilers provide major performance enhancements while maintaining the ease of use and flexibility that customers have come to expect with its predecessor the world renowned BeamScan NanoScan 2 scanheads are available to measure CW and pulsed beams across the entire spectral range from UV to infrared See Your Beam As Never Before The Graphical User Interface GUI of NanoScan is new Dockable and floatable windows plus concealable ribbon tool bars empower the NanoScan user to make the most of a small laptop display or a large multi monitor desktop PC Simple docked view Measured Beam Results From 1989 through 1996 John Fleischer past President of Photon Inc chaired the working laser beam width ISO DIN committee that resulted in the ISO DIN 11146 standard The final approved standard available in 13 languages The standard governs profile measurements and analysis using scanning apertures variable apertures area sensors and detector arrays NanoScan measures spatial beam irradiance profiles using scanning slit techniques The standard NanoScan uses the moving slit method approved by International Stand
396. th Beam Size 0 5mm 10mm M 200s Varies with wavelength waist size and location and M Damage Limits Camera 0 15 uW cm2 CW mode for a 10 mm input beam diameter 1 0 uJ cm pulse mode for a 10 mm input beam diameter Both of the above for an M 1 1064nm 1 CCD cameras can be damaged by power in excess of 100 mW cm or energy in excess of 100 mJ cm2 The M 200s employs a focusing optic While it may be that the laser input power or energy measures well below this damage threshold it can easily exceed these levels when focused onto the camera sensor Use caution and error on the side of safety CCD cameras can be costly to repair or replace Ordering Information Item Description P N M 200s Beam Propagation Analyzer M 200s FW M 200 software software license GRAS 20 Firewire camera short optical train automatic and manual SP90144 operation recommended for 266nm 1064nm wavelengths M 200s FW A M 200 software software license short optical train automatic and manual operation recommended for 266nm P90145 1064nm wavelengths GRAS 20 camera not included M 200sM FW Manual mode M 200 software software license GRAS 20 Firewire camera manual operation with a GRAS 20 SP90146 Firewire camera optical train not included Manual mode M 200 software software license manual operation with a Firewire camera GRAS 20 Firewire SP90147 camera and optical train not included Lens assy telecom 300mn fl M
397. the laser beam analysis and processing power of BeamGage The BeamGage automation interface allows developers to control BeamGage programmatically via a set of puppet strings known as the automation interface The automation interface was developed to provide the ability to base control decisions for a second application on results and behaviors recognized by BeamGage With this ability users can quickly and efficiently meet their manufacturing analysis goals with minimum human interaction The automation interface was designed to achieve two main goals First to allow the BeamGage user to programmatically do what they could otherwise do via the graphical user interface GUI Second to expose stable interfaces to the user that will not change causing breaks to their dependant code Interface examples for LabVIEW Excel and Net VB are included 3 2 1 3 BeamGage Enterprise Enterprise is an upgrade version of BeamGage Professional that has all of the BeamGage Standard and Professional features plus additional functionality 3 2 1 2 EMES Networking BeamGage Enterprise Edition BGE allows cameras to be accessed and shared over an Ethernet local area network LAN that shares a common domain 126 Y OPHIR Y Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport A Newport Corporation Brand
398. thru 399nm PH00370 167 HP ND1 400 thru 700nm PH00371 167 HP ND2 400 thru 700nm PH00372 167 HP ND3 400 thru 700nm PH00373 167 HP ND1 750 thru 890nm PH00374 167 HP ND2 750 thru 890nm PH00375 167 HP ND3 750 thru 890nm PH00376 167 HP ND1 900 thru 1100nm PH00377 167 HP ND2 900 thru 1100nm PH00378 167 HP ND3 900 thru 1100nm PH00379 167 HP ND1 1150 thru 1600nm PHO0380 167 HP ND2 1150 thru 1600nm PHO0381 167 HP ND3 1150 thru 1600nm PH00382 167 Il VI CO2 58 D8 WC H SP90160 205 I VI CO2 58 D8 WC V SP90161 205 VI CO2 BS 35 SP90062 205 QO OPHIR Spiricon Photon 01 08 2013 Photonics OPHIR Photonics OPHIR Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Terres Corporation Brand A Newport Corporation Brand A Newport Corporation Brand Product P N Page IR Phosphor Card 7FO1235A 44 77 Juno 7Z01250 87 101 L30A 10MM 7 02273 30 L30C SH 773434 50 L30C UA Consult Ophir representative 50 L30C UAU Consult Ophir representative 50 LAO 150 A 7202626 34 L40 150 A EX 7Z02614 34 L40 150 A LP1 7Z02685S 34 L50 150 A 7202633 34 L50 150 A BB 35 7202730 J2 L50 150 A LP1 35 72027265 32 L50 150 A PF 35 7202737 32 L50 150 A StarLink 787003 34 42 L50 300 A 7202658 35 L50 300 A IPL 7Z02651 35 L50 300 A LP 1 7Z026415S 35 L50 300 A PF 65 7202743 25 L150C UA Consult Ophir representative 53 L
399. tic convection ballistic convection ballistic Fiber Adapters Available see page 44 ST FC SMA SC ST FC SMA SC NA ST FC SMA SC Weight kg 0 6 0 6 0 6 0 6 Version V2 V2 V1 Part number Standard Sensor 7Z02626 7Z02685S 7Z02614 7Z02633 StarLink Sensor Direct USB link to PC p 42 787003 Notes a LP1 sensors have relatively large spectral variation in absorption and have a calibrated spectral curve at all wavelengths in their spectral range to the above specified accuracy Nova and Orion meters do not support this feature and when used with those meters accuracy will be 3 for 532nm 808nm 1064nm and 2940nm and 6 for other wavelengths in the spectral range 400 1100nm L40 150 A L40 150 A LP1 L40 150 A EX L50 150 A a90 po oiia 2x M3x3 deep 17 ADJUSTABLE 38 5 7 100 5x 3 5 6x 25 2x M3x3 deep 100 3 LA ADJUSTABLE amp 112 158 100 Q OPHIR Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 1 1 2 4 Medium Power Large Aperture Thermal Sensors Apertures 65mm 400mW to 300W Features Thin profile very large aperture a CW to 50W intermittent to 300W L50 300 A L50 300 A LP1 L50 300 A PF 65 L50 300 A IPL
400. to 13W without heat sink and 25W with heat sink see accessory pages 76 77 for heat sink and mounting post Notes e With the Laserstar Pulsar USBI Quasar and Nova Orion with adapter only 2 of the 5 pulse width settings are available For the PE C models the 30us and 1ms settings and for the PE BF models the 1ms and 10ms settings For sensors drawings please see page 71 OU OPHIR Photonics For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand 1 3 3 Wralasselss 70 1 3 3 High Energy Pyroelectric Sensors 100uJ to 40J Features PE50BF DIF C PESO0BF DIFH C Sensors with diffuser for high energies and high energy densities BF coating for highest damage threshold BB coating for spectral flatness Wide spectral range Measure YAG and harmonics and many more Rep rates up to 250Hz Measure lasers with pulse widths up to 20ms m PESOBF DIFH C sensor highest damage threshold PE50BB DIF C DIFFUSER IN DIFFUSER OUT 01 08 2013 Model PE5OBF DIF C PESOBF DIFH C PE50BB DIF C Use Complete calibration curve Highest damage Removable diffuser Spectrally flat threshold Diffuser Fixed Diffuser out Diffuser in Aperture mm 35 p46 033 Absorber Type BF with diffuser BB BB with diffuser Spectral Range um 0 19 2 2 2 94 0 19 20 0 4 2 5 Surface Reflectivity approx 25 5 15 Calibration Accuracy 3 3 3 Max Pulse Width Sett
401. ton and Graph type selections Stability Graph The more hits in one location the brighter the color Graph can be zoomed in and out manually or auto scaled Power measurement and statistics Graph with spot drawn to scale and market on position 01 08 2013 _ 2 OPHIR vhotais For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand Energy sensors 1 3 Bfelaiseyas O OPHIR gt ee For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand 1 3 Wrelaselss 62 01 08 2013 Energy Sensors Introduction Ophir has two types of energy sensors pyroelectric and RP Pyroelectric sensors are for measuring repetitive pulse energies and average powers at pulse rates up to 25000 pulses per second and pulse widths up to 20ms RP sensors are specialty items mainly for very long pulse widths and very high average powers that cannot be measured by pyroelectric sensors Note that single shot energy with pulse rates less than one pulse every 5s or so can be measured with thermal sensors described in the power sensor section Pyroelectric Sensors ice Pyroelectric crystal thickness lt 1mm Pyroelectric type sensors are useful for measuring the energy of repetitively pulsed lasers at up to 25 000HZ and are sensitive to low energies They are less durable than thermal types and t
402. top of each other and secured A set of 6 filters is provided that can achieve attenuation anywhere from ND 0 3 to ND 8 The LBF 50 is especially useful for CS or C mount cameras with the CCD recessed way below the surface The filters are recessed into the camera thus saving thickness as shown in the illustration to the right LBF 50 filter assembly LBF 50 on C mount camera Y OPHIR Y Spiricon Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand Newport Corporation Brand Transmission vs Wavelength These neutral density or ND filters do not have a flat response in attenuation vs wavelength See the graph for typical transmission vs wavelength characteristics Specifications Item ND1 ND2 ND3 LBF 50 Nominal ND vis l 23 o3 07 123 4 Clear Aperture O19mmM O12mm Damage threshold 5W cm 1J cm for ns pulses Continuously Variable Attenuator TRANSMISSION 900 1100 1300 1500 1700 1900 2100 2300 wavelength um For maximum ease of use there is the continuously variable attenuator that can vary its attenuation over a very wide range just by pushing and pulling the filters laterally The attenuator consists of two opposite wedges of ND glass The surfaces are arranged so that no parallel surfaces face each other so as to eliminate interference effects The variable att
403. tput to scope to see every pulse up to the maximum frequency of the sensor Fiber Adapters To mount fibers to sensors you need an adapter bracket and fiber adapter All ber adapters are compatible with the adapter bracket selected Fiber Adapter Brackets Mounting brackets to allow mounting fiber adapters to pyroelectric sensors PE Sensor Family Type Bracket P N Distance from fiber detector PD10 C PD10 pJ C 7Z08275 10mm PD10 IR pJ C PE50 C PE50BF C 7Z08270 15mm PES C PE10 C PEOBF C 7Z08269 10mm PE25 C PE25BF C Fiber Adapters Fiber adapters for mounting to above brackets SC type ST type FC type SMA type For all PE sensors above 7Z08227 7Z08226 7208229 1601236 Beam Splitter Assembly Beam Splitter Assembly to measure pulsed laser sources 7217001 too energetic for direct measurement The reading with the Beam Splitter can be calibrated by setting the laser to a lower energy that will not damage the sensor and then taking a measurement with the beam splitter and without and taking the ratio Q OPHIR 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 1 3 6 1 Accessories for Pyroelectric Sensors Continued Nova PE C Adapter Mounting Post Damage Threshold Test Plates Nova PE C Adapter PE C to PE Size Adapter IR Phosphor Card Shock Absorbing Mounting Post vibration and prevent false triggering at low en
404. tral range 193 1100nm Optional attenuators and fiber adapters available Battery or wall cube operation Description The FPS 1 fast photodetector is a compact easy to use very fast photodetector with wide spectral response It is used to measure the temporal pulse shape of laser pulses It has two modes of operation Into 500hm load for ns high peak power pulses and 10kOhm load for longer lower peak power pulses 1 3 6 2 Bielawelss In order to adjust the input intensity to the level appropriate for the detector you may scatter the laser light off of a white matt surface and back off till the appropriate intensity is reached Alternatively or in addition you may procure the ND attenuators listed below which may be stacked Specifications of the FPS 1 Fast Photodetector Detector Silicon PIN photodiode Spectral Range 193nm 1100nm Detector Area 0 8mm Wavelength of Peak Sensitivity 720nM Spectral Response See graph below Performance Specs Into 50Q load Into 10kQ load Sensitivity at Peak Wavelength 0 15V for 1W cm input 60V for 1W cm input Risetime 10 90 1 5ns 3us Maximum Output Voltage 10V Power Supply 12V A23 alkaline battery 40 hours lifetime Also can be operated from 12VDC wall cube power supply The power supply can be ordered from your local distributor Input Direct beam or from fiber connection Dimensions See drawing Thread Front flange is threaded with male SM1 thread Sensor Part Number FPS 1 fast photodio
405. trance Aperture 3 5mm 9mm 9mm Slit Size 1 8um 5um 25um 1 e Beam Diameter Range 4um 2 3mm 20um 6mm 100um 6mm Spatial Sampling Resolution 5 3nm 18 3um 5 3nm 18 3um 5 3nm 18 3um Profile Digitization 16 bit 16 bit 16 bit Scan Frequency 1 25 2 5 5 10 20Hz 1 25 2 5 5 10 20Hz 1 25 2 5 5 10 20Hz Power Aperture User calibrated User calibrated User calibrated Power Aperture OD Metallized Quartz 200mW Metallized Quartz 200mW Metallized Quartz 200mW Laser Type CW or Pulsed CW or Pulsed CW or Pulsed Operating Range See Operating Space Chart in Appen See Operating Space Chart in Appen See Operating Space Chart in Appen dix C of User s Manual dix C of User s Manual dix C of User s Manual Damage Threshold see Operating Space Chart in Appen see Operating Space Chart in Appen see Operating Space Chart in Appen dix C of User s Manual dix C of User s Manual dix C of User s Manual Rotation Mount Standard see drawing in Appendix B Standard see drawing in Appendix B Standard see drawing in Appendix B of User s Manual of User s Manual of User s Manual Scanhead Dimension See Mechanical Drawing in Appendix See Mechanical Drawing in Appendix See Mechanical Drawing in Appendix B of User s Manual B of User s Manual B of User s Manual 1 Assumes Gaussian TEM00 Beam 2 Pulsed Operation Limited to Beam Diameter gt 100uUm and pulse repetition rate 5kHz OU OPHIR Photon Photonics For la
406. troduction to Camera Based Profilers Beam Attenuating Accessories A camera based beam profiler system consists of a camera profiler software and a beam attenuation accessory Spiricon offers the broadest range of cameras in the market to cope with wavelengths from 13nm extreme UV to 3000 um in the long infrared Both USB and FireWire interfaces are available for most wavelength ranges providing flexibility for either laptop or desktop computers BeamGage Profiling Software Power Meter Optional Power Sensor Optional Laser Example of Beam Attenuator 2 wedge beam splitter with adjustable ND filters Camera BeamGage the profiling software comes in three versions Standard Professional and Enterprise Each builds off of the next adding additional capability and flexibility needed for adapting to almost any configuration requirement Spiricon also has the most extensive array of accessories for beam profiling There are components for attenuating filtering beamsplitting magnifying reducing and wavelength conversion There are components for wavelengths from the deep UV to CO2 wavelengths Most of the components are modular so they can be mixed and matched with each other to solve almost any beam profiling requirement needed Acquisition and Analysis Software The BeamGage software is written specifically for Microsoft Windows operating systems and takes full advantage of the ribbon base multi window environment The softwa
407. ts 193 360nm radiation to visible This plate SPZ17019 TS is at the object plane of the 4X expander so it produces a 4X enlarged image on the CCD C 6X expanding microscope objective Screw optical assembly that images the plane 16mm in front of the lens onto the CCD while SPZ08257 enlarging it 6X Fits 4 5mm recess and CS mount cameras Needs spacer assy below 7 L 12X expanding microscope objective Screw optical assembly that images the plane 6mm in front of the lens onto the CCD while SPZ08259 enlarging it 12X Fits 4 5mm recess and CS mount cameras Needs spacer assy below 22X expanding microscope objective Screw optical assembly that images the plane 2 6mm in front of the lens onto the CCD while SPZ08260 av enlarging it 22X Fits 4 5mm recess and CS mount cameras Needs spacer assy below ap Spacer assy for objectives Spacer assembly for above One only needed for all expanders above SPZ08261 aa Beam splitter for expanders above 45 degree angle wedge beam splitter which mounts onto beam expander Reduces beam intensity SPZ17027 by 20 times For spectral range 190 2500nm Introduces 35mm extra beam path to object plane IT Additional beam splitter for above Additional beam splitter to mount to 1st beam splitter SPZ17026 IT MM 178 Y OPHIR Y Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics eee Photonics A Newport Corporation Brand Ga Corporation Brand A Newpor
408. ts PH00243 NH PYRO 20 25 STD Head only NanoScan Pyro 20mm aperture 25um slits PH00413 NH PYRO 20 25 PRO Head only NanoScan Pyro 20mm aperture 25um slits PH00042 Software Upgrades NSv2 STD to NSv2 PRO Upgrade NanoScan v2 Standard version software to the PRO version This upgrade opens the NanoScan PH00417 Upgrade automation feature for those users wanting to integrate or develop their own interface using Visual Basic for Applications to embed into such applications as LabView Return scanhead to factory NSv1 to NSv2 STD Upgrade For those NanoScan users with pre v2 software approx before July 2012 they can upgrade their PH00418 hardware to v2 STD capability and can run the new software Automation capability is not available in v2 STD Once upgraded the legacy software will run but the automation feature will be disabled in v2 NSv1 to NSv2 PRO Upgrade For those NanoScan users with pre v2 software approx before July 2012 they can upgrade their PH00419 hardware to v2 PRO capability and can run the new software Automation capability is included in v2 PRO Once upgraded the legacy software will run including the automation capability in v2 Legacy Software Purchase the legacy V1 47 NanoScan software with licence and operations manual to PRO scanheads to PH00420 use the older software return scanhead to factory Q OPHIR Photon Photonics For latest updates please visit our website www ophiropt com photonics seer ens OLS 2013
409. u laser and average headers Energy Limits Screen Energy threshold m Pulsed energy sensors single or repetitive and thermal sensors single shot only m Frequency measurement with pulsed energy sensors Limits screen with bright colored warning pera ane N i eT oS D EN i Lauer 431 j leta begged ISEI avory pulit a nergy Logging Screen n S GN e VU m Pyroelectric and thermal sensors Present J Viner hih gt Continuous scroll with up to 100 points on screen Paane var ation a pulse to pulse m Full statistics m Store data onboard and recall Reset Zoom Exit ooo TE Choose analog _ Set startup needle screen configuration Peg Additional Functions Laser tune screen with continuous graph ua m Press the menu choice on the nae Adjust sensor ormallze so presen librati main screen and many more reading 16 1 00 calibration options pop up as shown Enter beam diameter and read in units of W cm or J cm Attenuate Adjust sensor Put in factor to read input power Limits PepPonbe UME with attenuator or beam splitter Set for alarm if preset min or Adjust power meter max limits exceeded Return to parameters previous menu Specifications Power Meter Brilliant color TFT 320 x 240 pixel graphics LCD Large 16mm digits High resolution analog needle also can be chosen Features Many screen features including power with multicolor bar graph energy average exposure freque
410. ucts RoHS Almost all Ophir and Spiricon Laser measurement products are now RoHS compliant The few products that are not ROHS are specified as such in the ordering information 3 De A Newport Corporation Brand ewport Corporatio For latest updates please visit our website www ophiropt com photonics Ophir Power and Energy Meters Versatility for Every Application Ophir sensor power meter and computer interface system means that virtually any sensor can work plug and play with any power meter or computer interface Ophir has the widest range of sensors on the market with the highest performance so almost any measurement need can be accommodated The measurement results can also be used in many ways on the power meter screen stored on board sent to PC with results presented in many ways and on several platforms Pyroelectric Sensors Thermal Sensors Photodiode Sensors Energies pJ to Joules Powers mW to kW and Powers pW to Watts Rep rates to 25kHz single shot energy FT r lt lt s l Computer Interfaces Power Meters with USB Bluetooth with USB RS232 CMIMIN Ne ge USB Interface Pulsar basic channels 4 2 1 Nova Il general Quasar Juno Nova Laser Star wireless compact compact 2 channel Software Solutions StarLab LabVIEW Starcom COM Object 5 Y OPHIR aoa For latest updates please visit our website www ophiropt com phot
411. um power is also limited by maximum output voltage where output voltage is at most 2V less than input voltage Note b 4 pin Molex connections Voltage Voltage Analog signal out Ground 6 pin Molex connections RS232 input Ground Voltage Analog signal out high low voltage or switch input when used RS232 output Note c Calibrated at customer selected wavelength 150C SH 150C UA 150W UA SS m Aa ener 58 2x M3x5 deep Z 50 8 14 5 19 4 2 sides Bi t B MOUNTING THREADS 018 JE 918 F gt i e e he Y Zl 3 mi i TETT f i MOLEX A MOLEX I MOUNTING HOLES ee 22 01 2065 E 22 01 2065 4x M4x8deep eo 13 P 38 MOUNTING THREADS 50 38 9 5 4 2x 1 8 27 NPT WATER CONNECTIONS 1 5 METER CABLE TO OPHIR SMART CONNECTOR 01 08 2013 AA OPHIR Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 1 1 5 1 Standard OEM Thermal Sensors 0 2W to 300W Features Conduction and water cooled Spectrally flat m UA version can give analog voltage output or digital RS232 output and can measure power or energy Can also have multiple switchable ranges and or multiple switchable wavelengths m UAU version is similar to the UA version but operates via the USB terminal of the PC L150C UA L150C UAU L250W UA L250W UAU L300W UA L300W UAU The
412. umber FL250A RP 0 01 Min Max Std Dev L1500W LP1 RP High power pulsed lasers LP1 0 6 1 1 06 1 1 p50MM 10W to 1500W 1500W 300W 700 6 Za 5 at 800nm and 1064nm 2 10W 200J to 150mJ 200J to 1J 5 150m4J in repetitive mode 500m4J in single shot mode 200 8 Pulse Width J cm pps lt 10us 0 05 15000 0 5ms 20 1400 5ms 120 150 100ms 2000 7 1 us 0 3V for 1kW peak power at 1064nm 0 01 Min Max Std Dev Sample to 15kHz every pulse to 1000Hz in turbo mode fan 1 2 V1 7Z02921 water 14 7Z02919 L1500W LP1 RP 112 105 40 DC Power S ADJUSTABLE upply Socket 106 152 ADJUSTABLE 122 168 100 75 1 3 4 Byelaisvelss ie Q OPHIR __ Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand 01 08 2013 Maximum Laser Repetition Rate for a Given Pulse Width Setting for RP Heads Maximum Pluse Width Setting ms 0 01 0 1 1 10 100 10000 100000 10000 1000 100 Maximum Repetition Rate Hz
413. umber of Elements 124 x 124 Interface Style USB 2 0 Interface Style Firewire 1394a Windows 05 support Windows 7 32 Vista 32 or XP 32 Pro Windows 05 support Windows 7 32 64 Vista 32 64 or XP 32 Pro 124 Y OPHIR Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand BeamGage Standard Unique Features Power Energy Calibration Using the USB output from select Ophir power energy meters the BeamGage application will display measured power energy values from the full range of Ophir thermopile photodiode and pyroelectric sensors Pulsed lasers can be synced up to 100HZz or the frame rate of the triggered camera whichever is less This is the first time in the industry a laser power meter has been married to a laser beam profile system BeamGage is the only product to integrate profiling and power meter measurements BeamMaker Numerical Beam Profile Generator BeamGage contains a utility BeamMaker that can synthetically generate beam profile data by modeling either Laguerre Hermite or donut laser beams in various modal configurations BeamMaker permits the user to model a beam profile by specifying the mode size width height intensity angle and noise content Once generated the user can then compare the theoretically derived measurements to measurements i
414. ured divergence is equal to M times the embedded divergence Therefore when the beam diameter at this location is minimized the divergence is at its minimum and the M of the laser should then be optimized After this real time adjustment the full M measurement can be done to generate the required parameter values This method makes the NanoModeScan an even more valuable tool for the final setup of lasers on the manufacturing floor by decreasing the time it takes both to adjust the laser system and to make the measurements required for quality control documentation NanoModeScan Specifications Sensor Detector Scan head Travel 500mm Optical Axis Height 140 170mm Standard Lenses 200mm EFL BK 7 plano convex Broadband AR Coated 400mm EFL BK 7 plano convex Broadband AR Coated UV through long IR lenses available Optional Lens 200mm FL fused silica for UV coated for wavelength of use 350mm FL fused silica for UV coated for wavelength of use 7 190mm FL IR lens for 10 6um wavelength Minimum Spot Size See scan head specifications Computer Electrical Source Power See scan head specifications File Saving and Data Logging Data files ASCII Files AC Power 110V 60Hz standard 220V 50Hz optional Communication RS 232 Interface or USB to RS 232 adapter required Mechanical Dimensions in mm NanoModeScan Linear Stage 812 X 102 x 78 Photon Motion Controller 273 x 89 x 57 Removable Light Shield 787 X 777 X 110 Weight Na
415. ures of the software You can read files saved LD8900R Software Viewer PH00439 Fiber Mount FC Plate and mount for a single mode fiber with FC connector Label on plate includes reference distance PH00189 between source and datum plane Fiber Mount SC Plate and mount for a single mode fiber with SC connector Label on plate includes reference distance PH00190 between source and datum plane Fiber Mount ST Plate and mount for a single mode fiber with ST connector Label on plate includes reference distance PH00191 between source and datum plane Fiber Mount BF Plate and mount for a single mode fiber without connector Label on plate includes reference distance PH00192 between source and datum plane Option to Fiber Mount BF Optional 4 Fiber Ribbon Cartridge for the Fiber Mount BF Bare Fiber Requires BF PH00193 Ribbon Extended Cable Option EXT Cable lengths extended PH00184 Cable NIST Reference Standard N A Reference Standard traceable to NIST for use with Goniometric Radiometer Far Field profilers i e PH00188 Q OPHIR Photonics A Newport Corporation Brand Newport Corporation Brand LD8900 and or LD8900R Data provided N A and Angular Widths at 50 13 5 and 5 clip levels with standard deviation with a recorded exact source to aperture distance NIST reference standard includes LD source Single Mode Test Fiber Required Mounting Plate in a storage case Photon For latest updates please visit our website
416. useful gain for saturation test and maximum useful gain for lowest signal test DN 2 May be useable for wavelengths below 350nm but sensitivity is low and detector deterioration may occur Therefore UV image converter is recommended Although our silicon cameras have shown response out to 1320nm it can cause significant blooming which could lead to 40 significant errors of beam width measurement We would suggest our XC130 InGaAs camera for these wavelengths to give you the best Cc measurements lt 3 This is the damage threshold of the filter glass of the filters Assuming all filters mounted with ND1 red housing filter in the front Distortion of the beam may occur with average power densities as low as 5W cm aA q e e e 41 OPHIR Y Spiricon Photonics For latest updates please visit our website www ophiropt com photonics OPHIR Photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand Newport Corporation Brand 2 N lt L z O Q aa 142 3 2 3 2 190 1100nm Firewire Silicon CCD Cameras Models GRAS 20 Features GRAS 20 m 61dB true system dynamic range 14 bit with BeamGage m High speed electronic shutters m Exclusive Ultracal available for ISO conforming accuracy m Flexible external trigger and strobe output for synchronization with laser pulses m Available with BeamGage software GRAS 20 GRAS 20 1550 1 32 UN C Mount
417. user ADJUSTABLE 90 139 ADJUSTABLE 90 139 OU OPHIR __ Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand UA t NN U N mM E 71 01 08 2013 1 3 3 High Energy Pyroelectric Sensors 10pJ to 40J PE50 DIF ER C PE100BF DIF C DIFFUSERIN DIFFUSER OUT DIFFUSERIN DIFFUSER OUT Por Features Removable diffusers m PE50 DIF ER C mainly for NIR lasers a m PE100BF DIF C for very large beams m Rep rates up to 10kHz Cc Measure lasers with pulse widths cA up to 20ms oo mM Model PE50 DIF ER C PE100BF DIF C Use Mainly for 1064nm 2 1m and 2 94um Very large aperture m Diffuser Diffuser out Diffuser in Diffuser out Diffuser in Aperture mm p46 033 p96 p85 Absorber Type Metallic Metallic with diffuser BF BF with diffuser Spectral Range um 0 19 3 0 4 3 0 15 3 0 4 2 5 Surface Reflectivity approx 50 50 20 50 Calibration Accuracy 3 3 3 3 Max Pulse Width Setting 2us 30us 500Us Ims 5ms 2us 30us 500us Ims 5ms ims 2ms 5ms 10ms 20ms Ims 2ms 5ms 10ms 20ms Energy Scales 10Jto 10Jto 10Jto 10Jto 10Jto 30Jto 30Jto 30Jto 30Jto 30Jto 10Jto 10Jto 10Jto 10Jto 10Jto 40Jto 40J to 40J to 40J to 40J to 200uJ 200K 2mJ 2mJ 2mJ 600W 600W 6mJ 6mJ 6m 2mJ 20m 20m 20m 20mJ 40m 40mJ 40mJ 40m 4
418. usly see Capture Options below a Trigger In from laser Trigger pulses supplied to the camera a Strobe Out to laser Strobe pulses output from the camera a Video Trigger Frame captured and displayed only when the camera sees a signal greater than a user set level Capture options a Capture options are redefined and are approached in a different manner than older products The items listed below will allow for all of the previous methods but with more flexability than ever before a Results Priority Results priority will slow the capture rate to be in sync with the computational results and display updates Frame Priority Frame priority will slow results and display updating to insure that frames are collected and stored in the frame buffer as fast as possible replaces block mode Stop After Will collect a set number of frames and then stop replaces Single Shot mode a Periodic Will collect frame at a programmed periodic rate a Periodic Burst Will collect frames in a Burst at programmed periodic rates Post processing is still available but is done via a different mechanism and is limited to only data file sources PC computer running Windows7 32 64 or XP 32 Pro Laptop or Desktop GHz Pentium style processor dual core recommended Minimum 2GB RAM 4GB required for Lw11058 camera Accelerated Graphics Processor Hard drive space suitable to hold the amount of video data you expect to store 50 100 GB recommended
419. ution head featuring Si detector 63 5mm diameter head with rotation mount 9mm entrance aperture and matched pair of 25 micron wide slits Use from 190nm to wavelengths lt 1micron Not for 1 06micron wavelength PHO0421 PHO0422 PH00423 NS2 Ge 3 5 1 6 STD NS2 Ge 9 5 STD NS2 Ge 9 25 STD NanoScan2 Ge Detector 3 5mm aperture 1 8micron slits High resolution head featuring Germanium detector 63 5mm diameter head with rotation mount 3 5mm entrance aperture and matched pair of 1 8 micron wide slits Use from 700nm to 1 8micron wavelength NanoScan2 Ge Detector 9mm Aperture 5 0micron slits High resolution head featuring Germanium detector 63 5mm diameter head with rotation mount 9mm entrance aperture and matched pair of 5 micron wide slits Use from 700nm to 1 8micron wavelength NanoScan2 Ge Detector 9mm Aperture 25 micron slits High resolution head featuring Germanium detector 63 5mm diameter head with rotation mount 9mm entrance aperture and matched pair of 25 micron wide slits Use from 700nm to 1 8micron wavelength PH00424 PH00425 PH00426 NS2 31 3 5 1 8 PRO NS2 Si 9 5 PRO NS2 51 9 25 PRO Software includes Activex automation feature NanoScan2 Silicon Detector 3 5mm aperture 1 8micron slits High resolution head featuring Silicon detector 63 5mm diameter head with rotation mount 3 5mm entrance aperture and matched pair of 1 8 micron wide slits Use from 190nm to wavelengths lt 1micron Not for
420. v 4 Network multiple cameras multiple versions of BeamGage External trigger for synchronization with laser pulses Gevicam Ma peneector Plane Coumi ear I H i i gp to j H EF Lp ii nw i F f 1 i Active ares Tit tha Gig E Cameras for use with Laptop or Desktop PC Item Specification Model Gevicam Application 1 1 8 format high resolution networkable long cable distances adjustable ROI Spectral Response Maximum beam size Pixel spacing Number of effective pixels Minimum system dynamic range Linearity with Power Accuracy of beam width Frame rates Shutter duration Gain control Trigger Photodiode trigger Saturation intensity Lowest measurable signa Damage threshold Dimensions and CCD recess Image quality at 1064nm Operation mode Software supported PC interface Minimum host system requirements Windows OS support 190 1100nm 7 16mm H x 5 44mm V 44um x 4 4um 1600 x 1200 57 lt dB full speed full resolution min gain 1 2 17fps full resolution 7 5fps optional faster rates with binning 60ms 17fps 133ms 7 5fps 33dB 5V TTL 2usec min positive pulse rising edge triggered N A 0 3uUW cm 0 5lux 17fps 50W cm 0 1J crm2 with all filters installed for lt 100ns pulse width 34mm x 34mm x 69mm CCD recess 17 5mm below surface Pulsed with video trigger good Pulsed sync
421. ve powers on the order of 5 to 30mW and most photodiode detectors saturate at about 2mW the PD300 sensor has been constructed with a built in filter so the basic sensor can measure up to 30mW without saturation With the removable extra filter the PD300 sensors series can measure up to 300mW or 3W depending on the model The Ophir power meter unit amplifies this signal and indicates the power level received by the sensor Due to the superior circuitry of the Ophir power meters the noise level is very low and the PD300 series sensors with Ophir power meter have a large dynamic range from picowatts to watts The PD300 is shown schematically below The PD300 and PD300 3W have the exclusive patented dual detectors connected back to back which eliminate any signal illuminating both detectors equally background light Laser hits 1 Removable filter Built in filter Photodiode 1 Photodiode 2 Calibration and Accuracy The sensitivity of various photodiode sensors varies from one sensor to another as well as with wavelength Therefore each PD300 sensor is individually calibrated against a NIST standard which has been calibrated at several nm intervals over the entire spectral range The calibration is done over the entire spectral range against the NIST standard using a computer controlled monochromator Since the instruments are calibrated against NIST standards the accuracy is generally 3 over the wavelength range the calibration has bee
422. ver the square of the magnification The system can be supplied with a lens for the user specified wavelength of use For viewing VCSEL junctions single mode fibers and large long wavelength LD junctions there is an optional 100 1 objective lens option producing diffraction limited performance from 400 700nm with a working distance of approximately 0 25 0 35mm and Numerical Aperture is 0 90 From 700 1600nm this lens produces near diffraction limited performance NanoScan Near Field Profiler Systems Parameter NFP VIS NFP 980 NFP 1550 NFP Pyro Tester Wavelength Range 400 700nm 700 1100nm 1300 1700nm 190 gt 20um lt 360nm optional Lens Spread Function 0 49um 1 1um 2 6um Maximum Source 140um 140um 200um Objective Focal Length 3MM 3MM 5 1mm AT tle Jent Objective Rear Focal Distance 160mm 160mm 207mm ma eee oat EMC Objective Numerical Aperture 0 85 0 85 0 48 p Objective Magnification 60 01 00 60 01 00 40 01 00 NanoScan Model NSSI 9 5 NSGE 9 5 NSGE 9 5 NSPyro 9 5 Aperture Size 9mm 9mm 9mm 9mm Slit Width 5um 5um 5um 5um 3 Axis Stage Travel X across rail 13mm micrometer adjust Y normal to rail 6 5mm fine pitch actuator Z along rail 13mm micrometer adjust VU OPHIR QO Spiricon Photons For latest updates please visit our website www ophiropt com photonics a DPR Phoronis A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand Newport Corporation Brand Ordering Information Item D
423. w Pyrocam IIl detectors have been damaged by CW power but some have been ablated by high peak pulse energy 3 2 4 ERRIMEN 152 Y OPHIR Y Spiricon 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics mere noone A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand Newport Corporation Brand GENERAL SPECIFICATIONS FOR PYROCAM III Application UV and IR Spectral response 13 355nm 1 06 3000um Interchangeable windows Active area 124mm x 124mm See selection in Ordering Information section Element spacing 100um x 100um Number of elements 124x 124 Pixel size 85um x 85um CHOPPED CW OPERATION Chopping frequencies 24Hz Optional chopper 48Hz Sensitivity RMS noise limit 220 nW pixel 24Hz 320 nW pixel 48Hz 2 2 mW cm2 24Hz 3 2 mW cm2 48Hz 45 nW Hz1 2 pixel 1Hz Noise equivalent power NEP 2 2W cm 24HZ Saturation power 3 2W cm2 48Hz Damage total power Over entire array 2W Power density 8W cm 2 PULSED OPERATION Laser pulse rate Single shot to 1000Hz Pulse width 1fs 12 8ms Sensitivity peak noise limit 7nJ pixel 70uJ cm Saturation energy 10mJ cm Damage threshold 20mJ cm 1ns pulse OPERATING CONNECTIONS AND CONDITIONS Power 600mJ cm 1 us pulse 120 230 VAC 60 50Hz External Supply Operating temperature PHYSICAL DIMENSIONS Case Dimensions D
424. wavelengths including 1um to over 3000um 0 1THz to 300THZ For THz sources the sensitivity of the Pyrocam Ill is relatively low at about 300MW cm at full output With a S N of 1000 beams of 30mW cm2 are easily visible In addition with Spiricon s patented Ultracal baseline setting multiple frames can be summed to pull a signal out of the noise Summing 256 frames enables viewing of beams as low as 1 2mW cm2 With Terahertz research suddenly being a central topic of interest the Pyrocam III becomes an invaluable aid in this exciting research Otherwise scientists working on Terahertz research have no easy way to characterize the profile or energy distribution of their lasers or sources THz laser beam at 0 2THz 1 55mm 3mW input power Broad Wavelength Response 19 frames summed The Pyrocam IIl detector array has a very broadband coating which enables operation at essentially all IR and UV laser wavelengths The curve ends at 100nm in the UV but X ray operation has been observed Likewise the curve ends at 100um in the far IR but the camera has been used at gt 3000um Thus you can use the Pyrocam III in the near IR for Nd YAG lasers at 100 1 06um and for infrared fiber optics at 1 3um and 1 55um Use the Pyrocam Ill for HF DF lasers near 4um and for Optical Parametric Oscillators from 1 um to 10um It measures Free Electron Lasers between 10um and 3000um
425. wer Measurement Pose bm dct Sensor type and S N Sensor Settings Set measurement mode to Power Energy or Track Scroll to on screen functions Set measurement configuration Set display to Barchart Needle or Position Beamtrack Position and Size Screen Mema Jha Lire H 11 327 Tel GPP Suid EHE Sensor type S Setti ensor Settings nd E N A 0 30mm YY mm l Size 34iimm eon a Meade Diep oy Sup Set measurement mode to Power Energy or Track Set measurement configuration 97 O OPHIR ao For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Bra 01 08 2013 1 5 EKON GAVAGE 98 01 08 2013 Analog Needle Screen m Perfect for adjusting and maximizing laser power or energy m Persistent graphical display allows tracking of minimum maximum values measured m Large analog needle with small digital display as well Configuration Screen m Easy adjustment of all measurement configuration parameters Context sensitive help for selected parameter m Sensor and meter information provided Specifications Large Analog Needle with Persistence Min Max Indicators Scroll back to Mode Display and Setup keys I Press to zoom graph on present measurement HH e Battery Status i ae Indicator 1 921 Persistence is on Previous readings shown in gray L
426. ww ophiropt com photonics e OPHIR nonce OPHIR Photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand A Newport Corporation Brand Part number index P N Page P N Page P N Page P N Page 11402 001 189 7Z02411A 22 702744 36 PH00028 200 77023 52 7202412 23 702919 73 PH00030 166 78105 96 99 7202413 23 702921 73 PH00031 166 78300 94 99 7202418 43 77932 66 PHO0033 166 773434 50 7ZO2422A 26 7Z02933 66 PHO0034 166 781051 96 99 7202424 22 7202934 68 PHO0035 166 781052 96 99 7202426 22 7202935 67 PH00036 166 787000 28 42 7 Z02436 25 7202936 68 PHO0038 166 78 001 28 42 7202437 25 7202937 67 PH00039 166 78 002 28 42 7202438 25 7202938 66 PHOO040 166 78 003 34 42 7202439 25 7202939 69 PH00041 166 200 787004 30 42 7 Z02440 26 7202940 70 PH00042 166 200 78 005 39 42 7Z02505 78 7202941 69 PH00043 200 787006 30 42 7 Z02602 49 7202942 72 PH00044 200 78 007 32 42 7202614 34 7202943 70 PH00046 167 78 100 22 42 7202621 28 7202944 65 PH00049 167 787152 66 75 7202622 28 702945 65 PH00050 167 787153 68 75 7202624 29
427. www ophiropt com photonics OPHIR Photonics A Newport Corporation Brand LD 8900HDR Far Field Profiler The photonics community needs a method for very high dynamic range measurements of optical fiber waveguide and other optical components Advances in DWDM technology deployment of standard fibers and the development of specialty fibers all require more accurate characterization These high dynamic range measurements of irradiant light flux have been very difficult to obtain Photon has the solution our Goniometric Radiometer the LD 8900HDR Far Field Profiler Measurement Parameters The LD 8900HDR Far Field Profiler uses goniometric methodology to measure true 3 dimensional profiles of optical components with up to 93 dB dynamic range All measurements are taken with the emitting fiber planar waveguide laser diode or LED inserted directly into the center of the instrument s radial measurement area For optical fiber the far field distribution pattern is acquired without bending the fiber Bending the fiber can cause analysis and reporting inaccuracies Parameters measured for optical fiber are Mode Field Diameter MFD used to evaluate losses due to mismatch at connections of fibers and fiber components Effective Area Aeff used to assess non linear effects Numerical Aperture NA a measure of the angular width of the fiber output NA is equal to the sine of the half angle sin 0 2 at a specified percentage of the
428. x 14cm H 400 1100nm calibrated for 1064nm SP620U 1600x1200 pixel camera with 4 4um spacing USB2 Continuously variable 1 frame rate to 1 6 000 manual or automatic OdB to 27dB in 700 steps each step is 0 035dB Manual or automatic control Std Beam Cube 60Hz Auto synch with laser Beam Cube 620 20Hz Auto synch with laser Automatic gain and shutter control Peak and Centroid position tracking 2D and 3D contour map Sophisticated noise and background control Best fit to gaussian or top hat profile 3D display viewable from any angle or elevation Store and recall screens in single or video fashion 3 different measures of beam width of peak 4 sigma and 90 10 knife eee Save numerical data files of profiles Log data with time Full on line instructions and help Fully flexible screen ormat Pentium 4 2GHz 256 MB Memory Operating system Windows XP Service Pack 2 or Vista 32 Continuously variable filters actuated from outside the unit 6 O 22mm at entrance for converging beam 7mm for collimated beams Expanded 2 3X With no lens 1X 5um 200us resp time Maximum peak power 1000W average power statistics Can send unlimited number of points in real time to PC via USB Interface at gt 1000 point s Windows software provided for data analysis Notes a The power density limitation applies to any surface that the beam hits For Beam Cube since the object plane is outside the instrument focal spots of much highe
429. y RS232 adapter with 8 meter cable including software 781051 Laserstar IEEE Option IEEE GPIB adapter for Laserstar 78300 Carrying Case for Vega Carrying case 38x30x11 cm For power meter and up to three sensors 1J02079 Nova Il StarLite and Nova 99 Y OPHIR ome For latest updates please visit our website www ophiropt com photonics 01 08 2013 A Newport Corporation Brand Newport Corporation Bra PC Connectivity Options for Power Energy Measurement Sample data with Ophir Ophir power meter capable of on power meter at up to 4000 board storage of data of up to 250 000 gt points per second points and data storage rate of up to L 4000 points per second l Ophir sensor to USB interfaces with up to 4 channel connectivity n gt Ophir Pyroelectric Thermal and Photodiode sensors measure at 2 up to 25 000 points per second EEE O j f U ye 1 a 3 Transmi Ophir Quasar Transmit real time data to PC at up to 25 000 Transmit stored data or interface points s per channel sensor limited via USB real time data to PC via O with wireless i i USB or RS232 OL connectivity Transmit real time data to PC at 500 points per second via Bluetooth StarLab software data transmitted via USB or Bluetooth Starcom software data transmitted via RS232 153 00 StarLab software StarCom
430. yed Data Handling Data can be viewed on board or transmitted to PC On Board Non volatile storage of up to 54 000 data points in up to 10 files Max data logging rate gt 1500 points s Transmitted to PC Data transmission rate of 500 points s RS232 baud rate of 38400 Sensor Features Works with thermal pyroelectric photodiode and RP sensors Automatic continuous background cancellation with PD300 sensors Submicrojoule and multikilohertz capability with pulsed energy sensors Program Features Preferred startup configuration can be set by user User can recalibrate power energy response time and zero offset Ordering Information Item Description Ophir P N Laserstar Laserstar single channel universal power meter for thermal pyroelectric photodiode and RP sensors 7Z01600 Laserstar 2 Channel Laserstar with dual channel capability including ration and difference measurement 7201601 RS232 Cable for Laserstar Cable RS232 D9 D25 1 unit supplied with Laserstar 7E01121 Laserstar Battery Pack Laserstar NiMH Battery update Kit 7Z14006A Laserstar IEEE Option IEEE GPIB adapter for Laserstar see page 99 78300 1 Q OPHIR 01 08 2013 Photonics For latest updates please visit our website www ophiropt com photonics A Newport Corporation Brand Newport Corporation Brand 2 1 4 NOVA Compact and Durable Power Energy Meter Compact and durable Compatible with all Ophir sensors thermal pyroelectric and photodiode Not compatible with PE
431. ze can be applied with minimal diffraction Beams of up to 2X the above size can be applied but noticeable diffraction will occur Y OPHIR Spiricon 7 Photonics For latest updates please visit our website www ophiropt com photonics Soy eee ES 01 08 2013 A Newport Corporation Brand Newport Corporation Brand A Newport Corporation Brand 3 8 3 High Power Laser Profiler Kits for CO2 A portable solution for medium power lasers Up to 1000W CO Up to 31mm beam widths 16mm 1 e2 width Level set and shoot Easy operation The LPK CO Beam Profiler Kits consist of an A R coated reflecting wedge CaF filters beam telescope to reduce larger beams Firewire Pyrocam camera BeamGage software computer and interface card if required The kit is designed to be conveniently placed in a horizontal beam or under a down directed beam to measure raw beam characteristics amp stability The user must safely handle the 95 to 99 5 of the beam that passes through the wedge A PC style computer is required but not included See the BeamGage Software section for software features and calculations See the table below for specifications LPK CO 16 A N gt Model Beam Reduction Beam Sizes Wavelength Type of Attenuator Camera LPK CO 6 4 0 5 1X 1 0 6 4mm 10 6um 0 5 beam splitter assorted attenuators Pyrocam Ill lt LPK CO gt 6 4 5 0 1X 1 0 6 4mm 10 6um 5 beam splitter assorted attenuators Pyrocam Ill

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