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Optical Detectors Update

02 June 2026 Newsletter - GoPhotonics

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Top Optical Detectors
Date: 02 June 2026
 
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Top Optical Detectors
Photoconductive Antenna
750 nm - 850 nm, Terahertz Photoconductive Antenna for Imaging Applications
Photoconductive Antenna  from Terahertz Store

The T-Era-20D-800-Air from Terahertz Store is a Terahertz Photoconductive Antenna that operates at a wavelength of 750 nm - 850 nm (excitation). It delivers an average optical power of 1 mW - 15 mW and has a spectrum bandwidth of 2.5 THz. This photoconductive antenna is ideal for terahertz spectroscopy & imaging, sensing, and electronic chip fault analysis in THz time domain systems.
Download Datasheet Product Details
Photoconductive Antenna
780 nm LT-GaAs Photoconductive Antenna for Spectroscopy Applications
Photoconductive Antenna  from TYDEX

The PCA-D-50-7.2-780 from TYDEX is an LT-GaAs Photoconductive Antenna that operates at a wavelength of 780 nm. It delivers a maximum output power of 30 mW and has a pulse duration of 120 fs. This photoconductive antenna has a dynamic range of 60 dB (at 0.5 THz) and dark current of 0.2 mA. It is ideal for industrial terahertz imaging and spectroscopy system applications.
Download Datasheet Product Details
Photodetector
700 nm - 1100 nm, Photodetector for Photometry Applications
Photodetector  from Opto Diode Corporation

The ODA-6WB-100M from Opto Diode Corporation is a Photodetector that operates at a wavelength of 400 nm - 1100 nm. It has a frequency response range of 1000 Hz (at -3 dB) and sensitivity of 20 V/μW. This photodetector has an active area of 5.87 mm2 and a transimpedance gain of 100 MOhms. It is ideal for photometry & colorimetry, pulse oximetry, and bar code reader applications.
Download Datasheet Product Details
Photodiode
800 nm - 2600 nm, InGaAs PIN Photodiode for LiDAR Applications
Photodiode  from Marktech Optoelectronics

The MTSM2601SMF2-150 from Marktech Optoelectronics is an InGaAs PIN Photodiode that operates at a wavelength of 800 nm - 2600 nm. It has an active area of 1.5 mm and a responsivity of 1.24 A/W. This photodiode has a shunt resistance of 5.56 kOhm and quantum efficiency of 72%. It is ideal for high-speed optical communication, gas/water analysis, LiDAR, and medical applications.
Download Datasheet Product Details
Photomultiplier
230 nm - 700 nm, Photomultiplier for Single Photon Counting Applications
Photomultiplier  from Becker & Hickl

The PMCS-150-110 from Becker & Hickl is a Photomultiplier that operates at a wavelength of 230 nm - 700 nm. It has a detector quantum efficiency of 35% (at 350 nm) and dark count rate of 20 s-1. This photomultiplier has an IRF width of 100 ps or 120 ps and a count rate above 5 MHz (continuous) & 100 MHz (peak). It is ideal for time-correlated single photon counting (TCSPC) applications.
Download Datasheet Product Details
Featured Whitepaper
Featured Whitepaper
High Performance Test Equipment Assures LED Lighting Products Comply with Industry Standards
Manufacturers and users of LED lighting applications need to be assured that their products will be qualified according to a multitude of reliability and efficiency standards. Click here to read the full whitepaper.
Photoreflector
670 nm Infrared Photoreflector for Edge Detection Applications
Photoreflector  from Shinkoh Electronics

The KR1226 from Shinkoh Electronics is an Infrared Photoreflector that operates at a wavelength of 670 nm. It has a rise time of 70 µs and fall time of 95 µs. This photoreflector has a dark current of 1 nA and light current of 150 μA. It has a maximum leak current of 10 μA and reverse current of 10 μA. This photoreceptor is ideal for bar-code reader, edge detection & mark sensor of OCR applications.
Download Datasheet Product Details
Photoresistor
560 nm Photoresistor for Light Detection Systems
Photoresistor  from Nanyang Lida Optic-electronics

The GT36537 from Nanyang Lida Optic-electronics is a Photoresistor that operates at a wavelength of 560 nm. It has a light resistance of 18 kOhms - 50 kOhms and dark resistance of 2 MOhms. This photoresistor has an operating temperature of 30 deg - 70 deg and a resistance illumination coefficient of 0.7. It requires an AC supply voltage of 100 V and and consumes 50 mW of power. This photoresistor is ideal for light detection system applications.
Download Datasheet Product Details
Phototransistor
880 nm Silicon Phototransistor for Detection Applications
Phototransistor  from Optrans America

The PTC080M3B from Optrans America is a Silicon Phototransistor that has a peak sensitivity wavelength of 880 nm. It has a spectral range of 400 nm - 1100 nm, switching time (rise/fall) of 10 μs, and an angular response of ± 80 deg. This transistor has a C-E current of 1 mA and collector dark current of up to 100 nA. It is ideal for optical switches, detectors, and sensor applications.
Download Datasheet Product Details
Pyroelectric Detector
5 µm - 14 µm, Digital Pyroelectric Detector for Flame Detection Applications
Pyroelectric Detector  from Broadcom

The AFBR-S6EPY12111B from Broadcom is a Thin Film Digital Pyroelectric Detector that has a filter bandwidth of 5 µm - 14 µm. It has a 5 µm long-pass filter and offers high immunity to electromagnetic interference. This pyroelectric detector uses a digital current-mode read-out to reduce IR-emitter duty cycles and is ideal for gas sensing, flame & motion detection, and gesture recognition applications.
Download Datasheet Product Details
Terahertz Detector
50 GHz - 700 GHz, Terahertz Detector for Research Applications
Terahertz Detector  from Terasense Group

The Ultrafast Sub-THz Detector from Terasense Group is a Terahertz Detector that has a spectral range of 50 GHz - 0.7 THz. It has a response time of 150 ps & 2 µs and responsivity of 0.5 V/W & 10 V/W. This terahertz detector has a noise equivalent power of 1 nW/rt(Hz) - 2 nW/rt(Hz) and is ideal for terahertz imaging, non-destructive analysis, and scientific research applications.
Download Datasheet Product Details
Featured Article
Featured Article
What is Photon Echo?
Photon echo is a phenomenon in physics where a pulse of light is spontaneously emitted from a system of atoms previously irradiated by two coherent resonant light pulses. This emission is observed at a time shortly after the second pulse, and this timing closely aligns with the time between the two initial excitation pulses. Click here to read the full article.
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