| New Photonics Products this Week |
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| 520 nm Fiber Coupled Laser Diode | |
Laser Diode
from PhotonTec Berlin
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| The M520±10-2-D400/22-G3W-P from PhotonTec Berlin is a Fiber Coupled Laser Diode with a wavelength of 520 nm. It delivers an output power of 2 W and has a maximum spectral width (FWHM) of 10 nm. This laser diode has a slope efficiency of 21.6 W/mA and power conversion efficiency of 16%. It has a fiber pigtailed core diameter of 400 μm and numerical aperture of 0.22. This laser diode is available in a package that measures 52 mm x 43 mm x 20.1 mm. |
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| 808 nm Fabry-Perot Laser Diode for Optical Tweezer Applications | |
Laser Diode
from TOPTICA EAGLEYARD
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| The EYP-RWL Series from TOPTICA EAGLEYARD is a Fabry-Perot Laser Diode with a center wavelength of 808 nm. It delivers an output power of 400 mW - 450 mW and has a spectral width (FWHM) of 1 nm. This laser diode has a polarization extinction ratio of 18 dB and temperature coefficient of wavelength of 0.28 nm/K. It is ideal for pumping, communication, and optical tweezer applications. |
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| 1540 nm - 1560 nm, Pulsed Fiber Laser for LiDAR Applications | |
Laser
from BKtel Photonics
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| The HFL from BKtel Photonics is a Pulsed Fiber Laser that operates at a wavelength of 1540 nm - 1560 nm. It delivers an output power of up to 4 W and has a pulse width of 0.4 ns - 50 ns. This randomly or linearly polarized laser has a pulse energy of 50 μJ and repetition rate of 10 kHz - 2000 kHz. It is ideal for test & measurement, distance measurement, and LiDAR applications. |
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| 1534 nm DPSS Lasers for LiDAR & Instrumentation Applications | |
Laser
from RPMC Lasers Inc.
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| The KAUKAS SERIES from RPMC Lasers Inc. are DPSS Lasers that operate at a wavelength of 1534 nm. They have a pulse width of less than 11 ns and pulse energy of up to 3 mJ. These nanosecond pulsed lasers have a TEM00 spatial mode and are ideal for LiDAR, laser ranging, Laser-Induced Breakdown Spectroscopy (LIBS), metrology & instrumentation applications. |
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| 635 nm Red Line Laser for Laboratory Applications | |
Laser
from IMM Photonics GmbH
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| The IMM1618-635-1-L from IMM Photonics GmbH is a Red Line Laser that operates at a wavelength of 635 nm. It delivers an output power of 0.95 mW and has a beam divergence of 0.4 mrad. This single homogeneous laser produces a beam of diameter 0.7 mm x 80 mm. It uses plastic or glass optics and is ideal for measuring instruments, pointing, alignment lasers, laboratory instruments, and sensor applications. |
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| 940 nm Continuous Wave Laser Diode | |
Laser Diode
from Sheaumann Laser
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| The T-Series-M9-MM-940nm-100um-1.W from Sheaumann Laser is a Continuous Wave (CW) Laser Diode that operates at a wavelength of 940 nm. It delivers an output power of 1.5 W and has a slope efficiency of 1 W/A. This multimode laser diode has a beam divergence of 30 degrees (vertical far-field) and 9 degrees (horizontal far-field) at FWHM. It requires a threshold current of 300 mA, DC supply voltage of 1.7 V, and consumes 1.8 A of current. |
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| 1064 nm DPSS Laser Gain Module | |
Laser Gain Module
from Oriental laser
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| The GN500-E-5*182-CX-50 from Oriental laser is a DPSS Laser Gain Module with a central wavelength of 1064 nm. It delivers an output power of 500 W and has a lifetime of 10000 hours. This laser gain module has an Nd:YAG doping concentration of 0.60% and center height (Nd:YAG) of 50 mm. It has a diameter (Nd:YAG) of 5 mm and length (Nd:YAG) of 182 mm. This laser gain module has a threshold current of 7 A and current limit of 27 A. |
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| Laser Gain Module for Laser Manufacturing Applications | |
Laser Gain Module
from Geola
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| The GAP6D from Geola is a Laser Gain Module with a pumping energy of 300 J. It has a rod size of Ø6.3 mm x 100 mm and linear flashlamp size of 5 mm x 75 mm. This laser gain module is designed for use with Er:YAG, Er:YLF, Nd:Glass, Nd:KGW, Nd:YAG, Nd:YLF, Nd:YVO, and Yb:YAG laser rods. It has a beam height of 25 mm and is ideal for laser manufacturing applications. |
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| 1064 nm Laser Gain Module for Cascade Amplification Systems | |
Laser Gain Module
from Astrum LT
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| The NDYAG-QCW16-72-9 from Astrum LT is a Laser Gain Module that operates at a wavelength of 1064 nm. It has a peak pump power of 16.5 kW and pulse energy of 1.7 J. This laser gain module has a pulse length of 0.3 ms, repetition rate of 10 Hz, and small signal gain of 12.5. It is ideal for master oscillator power amplifier and cascade amplification system applications. |
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| 5 Megapixel CMOS Image Sensor for Machine Vision Applications | |
CMOS Image Sensor
from Gpixel Microelectronics Inc.
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| The GMAX3405 from Gpixel Microelectronics Inc. are 5 Megapixel CMOS Image Sensors that have a resolution of 2448 (H) x 2048 (V) pixels. They have a charge domain electronic global shutter in a 2/3" optical format that deliver a maximum frame rate of 264 fps. These CMOS image sensors are ideal for machine vision, logistics barcode readers & intelligent traffic system applications. |
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| 185 nm - 900 nm, Photomultiplier for Low Light Measurements | |
Photomultiplier
from MKS | Newport
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| The 77341 from MKS | Newport is a Photomultiplier that operates at a wavelength of 185 nm - 900 nm. It has a peak responsivity of 74 mA/W and peak wavelength of 400 nm. This photomultiplier has a current amplification of 1 x 107 and an active area of 8 mm x 24 mm. It has a rise time of 2.2 ns and transit time of 22 ns. This photomultiplier is ideal for low-light measurements. |
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| Silicon Photomultiplier for Imaging & Research Applications | |
Photomultiplier
from Broadcom
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| The AFBR-S4K33P6425B from Broadcom is a Silicon Photomultiplier that has an effective photosensitive area of 3 mm x 3 mm. It has an array size of 8 mm x 8 mm and array fill factor of 80%. This photomultiplier has a channel size of 3 mm x 3 mm and pitch of 3.36 mm. It is ideal for medical imaging, physics research, and analytical instrumentation applications. |
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| Photomultiplier for Flow Cytometry Applications | |
Photomultiplier
from ElectroOptical Innovations
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| The SiPM Module from ElectroOptical Innovations is a Photomultiplier that has a bandwidth from DC - 200 kHz to DC - 300 MHz (3 dB). It has a rise time of 4 ns and an output impedance of 50 Ohms. This photomultiplier features DC coupling and supports both analog & photon counting operations across all configurations. It requires a DC supply voltage of 5 V and is ideal for flow cytometry, microplate readers & TOF LiDAR applications. |
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| 1050 nm Spatial Light Modulator for Laser Marking Applications | |
Spatial Light Modulator
from Hamamatsu Photonics
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| The X15213-03CL from Hamamatsu Photonics is a Spatial Light Modulator with a wavelength of 1050 nm. It has a wavelength accuracy of ± 50 nm and light utilization efficiency of 97%. This spatial light modulator is ideal for optical beam pattern shaping, laser processing, laser marking, optical tweezers, wavefront aberration correction & metal 3D printing applications. |
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| 640 nm - 1100 nm, Spatial Light Modulator for Holography Applications | |
Spatial Light Modulator
from Thorlabs Inc
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| The EXULUS-HD3HP from Thorlabs Inc is a Liquid Crystal on Silicon (LCoS) Spatial Light Modulator that operates at a wavelength of 640 nm - 1100 nm. It has a display panel resolution of 1920 x 1200 pixels and an active area of 15.42 mm x 9.66 mm. This reflective spatial light modulator is ideal for adaptive optics, holography, interferometry, laser processing, and lithography applications. |
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| 2K SWIR Line-Scan Array Camera for Semiconductor Inspection Applications | |
Scientific & Industrial Camera
from New Imaging Technologies
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| The LiSaSWIR 2048 from New Imaging Technologies is a 2K SWIR Line-Scan Array Camera that has a resolution of 2048 x 1 pixels. It has a spectral response of 0.9 µm - 1.7 µm and pixel pitch of 8 µm x 8 µm. This InGaAs camera is ideal for applications such as semiconductor & solar cell inspection, food sorting, waste sorting, and hot glass inspection. |
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| 535 nm - 820 nm, Fabry-Perot Interferometer for Laser Spectral Analysis | |
Interferometer
from LD-PD Inc
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| The SFPI-500A(DP) from LD-PD Inc is a Fabry-Pérot Interferometer that has a spectral response of 535 nm - 820 nm. It has a free spectrum range of 1.5 GHz and resolution of less than 7.5 MHz. This scanning interferometer has a confocal Fabry-Perot optical cavity and is ideal for applications such as examining the fine structure of the spectral characteristics of continuous-wave lasers. |
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