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| | | Weekly Edition | | | Date: 13 February 2025 | | | |
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| New Photonics Products this Week | |
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| 632.8 nm Helium-Neon Laser for Microscopy & Spectroscopy Applications | |
Laser
from OptoSigma Corporation
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| The OSK-6328-18 from OptoSigma Corporation is a Helium-Neon Laser that operates at a wavelength of 632.8 nm. It delivers an output power of 18 mW, has a beam divergence of up to 1 mrad, and produces a beam of diameter 1 mm. This is ideal for confocal laser scanning microscopy, spectroscopy, digital imaging, metrology, industrial measurements, medical, and basic research applications. |
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| 532 nm Nanosecond Laser for Marking & Laser Ranging Applications | |
Laser
from Photonics Industries
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| The DX-532-15 from Photonics Industries is a Nanosecond Laser that operates at a wavelength of 532 nm. It delivers an average power of 15 W and has a pulse energy of 300 μJ (at 50 kHz). This laser has a pulse width of 10 ns - 15 ns (at 50 kHz), pulse repetition rate from single shot to 300 kHz, and is ideal for marking & scribing, PERC & solar cell, LiDAR & laser ranging, and silicon applications. |
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| 527 nm Green CW Laser for Scientific & Machine Vision Applications | |
Laser
from Power Technology Inc.
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| The DTL-413-1500 from Power Technology Inc. is a Green Continuous Wave (CW) Laser that operates at a wavelength of 527 nm. It delivers an output power of 1500 mW and has a spectral width of 4.5 cm-1 (at FWHM). This collimated laser has a peak-to-peak power stability of up to 2% and an RMS noise of 1%. It is ideal for military, defense, scientific, machine vision, and industrial applications. |
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| 5 µm - 15 µm, MIR Supercontinuum Source for Spectroscopy Applications | |
Supercontinuum Source
from TOPTICA Photonics
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| The FemtoFiber dichro midIR from TOPTICA Photonics is a Mid-Infrared (MIR) Supercontinuum Source that operates at a wavelength of 5 µm - 15 µm. It delivers an output power of 1 W and has an emission bandwidth above 400 cm-1. This vertically polarized supercontinuum source has a power stability of less than 1% and is ideal for mid-infrared spectroscopy and imaging applications. |
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| 760 nm Fabry-Perot Laser Diode for Spectroscopy Applications | |
Laser Diode
from TOPTICA eagleyard
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| The EYP-RWE-0760-02010-1500-SOT12-0000 from TOPTICA eagleyard is a Fabry-Perot Laser Diode that operates at a wavelength of 760 nm. It delivers an output power of 80 mW and has a tuning range of 752 nm - 772 nm. This laser diode has TEM00 mode with a beam divergence of 10 deg (parallel) and 28 deg (perpendicular) at FWHM. It is ideal for spectroscopy applications. |
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| 915 nm CW Multimode Laser Diode for Defense & Medical Applications | |
Laser Diode
from Sheaumann Laser
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| The CMC-915-2000-1 from Sheaumann Laser is a Continuous Wave Laser Diode that operates at a wavelength of 915 nm. It delivers an output power of 2 W and has a slope efficiency of 1 W/A. This multimode laser diode has a beam divergence of 30 degrees (vertical far-field) & 8 degrees (horizontal far-field) at FWHM. It is ideal for laser pumping, laser therapy, defense, and medical applications. |
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| 0.9 µm - 1.7 µm, InGaAs SWIR Image Sensor for Scientific Applications | |
SWIR Sensor
from Chunghwa Leading Photonics Tech (CLPT)
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| The FPA0640P15F-17-T2 from Chunghwa Leading Photonics Tech (CLPT) is an InGaAs SWIR Image Sensor that has a spectral range of 0.9 µm - 1.7 µm. It has a quantum efficiency fill factor (QEFF) above 70 % (at 1 µm - 1.6 µm) and an effective pixel array of 636 (H) x 508 (V) pixels. This SWIR sensor is ideal for near-infrared imaging, covert surveillance, and scientific applications. |
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| 850 nm GaAlAs Infrared LED for High Power Fiber Optic Applications | |
LED
from Texas Photonics
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| The TXPI 1000 from Texas Photonics is a GaAlAs Infrared LED that operates at a wavelength of 850 nm. It has a spectral bandwidth of 50 nm and delivers an optical output power of 3.5 mW. This LED has a reverse voltage of 5 V and capacitance of 70 pF. It has a rise time of 4 ns and fall time of 6 ns. This LED has internal lensing for efficient fiber coupling. It is ideal for high-power fiber optic applications. |
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| 265 nm - 322 nm, SiC Photodetector for Flame Control Applications | |
Photodetector
from ifw optronics
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| The JEA1B from ifw optronics is a Silicon Carbide (SiC) Photodetector that has a spectral range of 265 nm - 322 nm. It has a peak response wavelength of 300 nm and an active area of 1 mm x 1 mm. This photodetector has a field of view of ± 45 Grad and peak response of 0.12 A/W. It is ideal for optical measurement in UV-range with limited spectral range, and flame control applications. |
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| 650 nm - 1050 nm, UV-Grade Fused Silica Non-Polarizing Beamsplitter | |
Beam Splitter
from OPTOMAN
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| The PP-UVFS-25.4-3.0-NPBS5-AR177 from OPTOMAN is a Non-Polarizing Beam Splitter that operates at a wavelength of 650 nm - 1050 nm. It has a diameter of 25.4 mm and thickness of 3 mm. This UVFS beam splitter has a clear aperture above 80 % and surface quality of 10-5 scratch-dig. It has a surface flatness of up to lambda/6 (at 633 nm) and parallelism of less than 10 arcsec. |
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| Fiber End Face Interferometer for 2D & 3D Topography Applications | |
Interferometer
from NorthLab Photonics
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| The ProViewTM LD from NorthLab Photonics is a Fiber End Face Interferometer that has a resolution of 2560 (H) x 1920 (V) pixels. It has a fiber cladding diameter of 125 µm - 720 µm and field of view of 800 µm. This interferometer has an absolute accuracy of 0.03° standard deviation (above 400 µm) & 0.02° standard deviation (below 400 µm) and is ideal for 2D & 3D topography applications. |
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| Featured Article | | What is Raman Spectroscopy? | | Raman spectroscopy is a spectroscopic technique that utilizes scattered light to probe the vibrational energy modes present within a sample. It is named after the eminent Indian physicist C. V. Raman who pioneered its observation in 1928 alongside his collaborator K. S. Krishnan. Originally, the Raman effect was observed using sunlight and mercury arc lamps. Click here to read the full article. | | | |
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