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Optical Detectors Update

09 September 2025 Newsletter - GoPhotonics

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GoPhotonics
Top Optical Detectors
Date: 09 September 2025
 
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Top Optical Detectors
Photodetector
193 nm - 1100 nm, UV Silicon Photodetector for Measuring Temporal Pulse Shape
Photodetector  from MKS | Ophir

The FPD-UV-3000 from MKS | Ophir is a UV Silicon Photodetector that has a spectral range of 193 nm - 1100 nm. It operates at a wavelength (peak sensitivity) of 890 nm and delivers a maximum average power of 15 mW. This photodetector has an active area diameter of 2.55 mm and a rise/fall time of 3 ns. It has a bandwidth above 118 MHz and is ideal for measuring temporal pulse shape.
Download Datasheet Product Details
Photodetector
1530 nm - 1565 nm, Photodetector for RF Generation Applications
Photodetector  from Phase Sensitive Innovations

The D4 Series from Phase Sensitive Innovations is a Uni-Traveling Carrier (UTC) Photodetector that operates at a wavelength of 1530 nm - 1565 nm. It has a responsivity of 0.4 A/W and bandwidth of 25 GHz. This photodetector has a high linearity and is ideal for high-speed photodetection, photonic RF generation, multimode photodetection, and microwave photonic link applications.
Download Datasheet Product Details
Photodetector
800 nm - 1700 nm, InGaAs Avalanche Photodetector for Sensing Applications
Photodetector  from LD-PD Inc

The APD-100M-A from LD-PD Inc is an InGaAs Avalanche Photodetector that has a spectral range of 800 nm - 1700 nm. It has a bandwidth of 100 MHz and detector responsivity of 9 V/W. This photodetector has a transimpedance gain of 300K V/W and is ideal for optical fiber sensing, optical fiber communication, laser ranging, and spectrometry applications.
Download Datasheet Product Details
Photodiode
850 nm GaAs PIN Photodiode for Fiber Optic Communication Applications
Photodiode  from Coherent Corp.

The APA1201010000 from Coherent Corp. is a GaAs PIN Photodiode that operates at a wavelength of 850 nm. It has a 3dB-bandwidth of 20 GHz and data rate of up to 25 Gb/s. This single-channel photodiode has an aperture diameter of 40 μm and a responsivity of 0.6 A/W. It has a dark current of 3 pA and is ideal for datacom & parallel multimode fiber optical communication applications.
Download Datasheet Product Details
Photodiode
900 nm - 1700 nm, PIN Photodiode for Industrial Applications
Photodiode  from LD4B

The  PD4B-200-P20-1G-K from LD4B is a PIN Photodiode that operates at a wavelength of 900 nm - 1700 nm. It has a bandwidth of 1 GHz and responsivity of 1 A/W (at 1550 nm). This photodiode has a capacitance of 3 pF, dark current of 0.05 nA, and return loss of 16 dB & 30 dB. It has a fiber length of 20 cm - 100 cm and is ideal for scientific & industrial applications.
Download Datasheet Product Details
Featured Interview
Interview with Gustavo Rivas from Cybel, LLC
Interview with Gustavo Rivas from Cybel, LLC
GoPhotonics interviewed Gustavo Rivas, the Technical Sales Manager of Cybel, LLC. Gustavo Rivas is an electrical engineer from the District University of Bogota, over the past few years, his focus has been in the photonics industry including the fiber lasers and fiber amplifiers industry. Before Cybel, Gustavo also worked with other companies. Click here to read the full interview.
Photodiode
950 nm - 1650 nm, InGaAs Avalanche Photodiode for LiDAR Applications
Photodiode  from Phlux Technology

The PX01080-SM from Phlux Technology is an InGaAs Avalanche Photodiode (APD) that has a spectral response of 950 nm - 1650 nm. It has a gain above 100 and noise factor of up to 3.5. This APD has a temperature coefficient of breakdown voltage below 20 mV/K and is ideal for LiDAR, LRF, OTDR, free space communication, and optical / fiber sensing applications.
Download Datasheet Product Details
Photodiode
Single-Photon Avalanche Diode Sensor for Quantum Sensing Applications
Photodiode  from Singular Photonics

The Andarta from Singular Photonics is a Single-Photon Avalanche Diode (SPAD) Sensor that has a pixel pitch of 10.17 μm. It has a fill factor of 100% (with micro lenses) and pixel array of 512 x 512 pixels & 128 x 128 (macro pixels). This sensor is ideal for Raman spectroscopy, FLIM, time-resolved multispectral beam-scanned imaging, quantum sensing, and microscopy applications.
Download Datasheet Product Details
Phototransistor
800 nm Silicon Phototransistor for Industrial Equipment Applications
Phototransistor  from ROHM Semiconductor

The SML-H10TB from ROHM Semiconductor is a Silicon Phototransistor that operates at a wavelength of 800 nm. It has a light current of 2 mA - 4 mA and dark current of up to 0.5 µA. This phototransistor has a collector-emitter voltage of 32 V, collector current of 30 mA, and an emitter-collector voltage of 5 V. It is ideal for home appliance & industrial equipment applications.
Download Datasheet Product Details
Phototransistor
880 nm Silicon Phototransistor for Optical Switches & Detectors
Phototransistor  from Marktech Optoelectronics

The MTD8000M3B-T from Marktech Optoelectronics is a Silicon Phototransistor that has a peak sensitivity wavelength of 880 nm. It has a spectral sensitivity of 400 nm - 1100 nm and switching time (rise/fall) of 10 µs. This phototransistor has a collector-emitter current of 1 mA and is ideal for optical switches, optical sensors & optical detectors.
Download Datasheet Product Details
Phototransistor
750 nm Silicon Phototransistor for Optical Encoder Applications
Phototransistor  from Optoi

The OIT7C-NR from Optoi is a Silicon Phototransistor that has a peak responsivity of 750 nm. It has an optical pitch of 0.6 mm and electrical pitch of 1.27 mm. This phototransistor has a spectral bandwidth of 500 nm - 950 nm and gain of 600. It has a rise time of 10 μs and is ideal for optical encoders, 12-13 bit absolute encoders, optical receivers, and controls/drives applications.
Download Datasheet Product Details
Featured Article
Featured Article
What is Pockels Effect?
Pockels Effect is the linear electro-optic effect in which the refractive index of the medium is modified with respect to an applied electric signal or voltage. This effect was discovered by the German physicist Friedrich Pockels in 1893. It occurs only in non-centrosymmetric crystals, i.e., crystals with inversion symmetry. Click here to read the full article.
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