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Photon Doppler Velocimeter - PXIe
Doppler 1000 Series
The Quantifi Photonics Doppler PXIe module combines the key optical components for Photonic Doppler Velocimetry (PDV) measurements in a compact instrument to enable streamlined high-channel count PDV test setups.
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Laser Scanning FLIM Microscopes
DCS-120 laser scanner: Compact - Flexible - Precise. As technology leader in equipment and techniques for single photon counting, Becker & Hickl offers the DCS-120 systems that are complete laser scanning microscopes for fluorescence lifetime imaging (FLIM) since 2007. The systems use bh’s multi-dimensional TCSPC FLIM technology in combination with fast laser scanning and confocal detection or multi-photon excitation.
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Solar Simulator
Sun 3000 Class AAA
The Abet Gen II optical design, patent pending, dramatically increases the percentage of photons reaching the work plane.All electronics are packaged in the lamp house – no clutter of high power cables to deal with. Photofeedback and digital shutter timer are included.Standard maintenance, lamp or filter replacement, does not require any tools. Locking indicator dials on all the system controls provide for a reproducible and stable setup. A built-in beam imaging accessory assists in system alignment.
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HiCATT
The High-speed Intensified Camera Attachment (HiCATT) is designed for use with a high-speed camera. It increases the sensitivity of your camera and enables low-light imaging at frame rates up to 1 MHz (10 Mhz in burst)The technology in the HiCATT expands the dynamic range of your high-speed camera. At low light levels, even single photons can be detected. While at high light levels, overexposure can be prevented by very short exposures (down to 3 ns). These short exposures yield sharp images of fast moving objects.
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EMCCD Cameras
iXon Life
With the iXon EMCCD cameras, Andor have delivered a dedicated, truly high-end, yet accessible ultrasensitive scientific camera platform, designed specifically to drive the absolute best from EMCCD technology across all critical performance specs and parameters. Andor’s new iXon Life EMCCD platform is available exclusively for fluorescence microscopy applications and is engineered to deliver single photon sensitivity with absolutely unparalleled price/performance. Perfect for single molecule detection and live cell microscopy with minimized phototoxicity or photobleaching, but at a price more normally associated with back-illuminated sCMOS cameras.
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Hybrid Photon Counting Detectors
MYTHEN2 Series
MYTHEN2 detectors guarantee noise-free performance, maximum resolution, and outstanding signal-to-noise ratios for an extended energy range from 4 to 40 keV. These systems include two module sizes: 1K with 1280 strips, and 1D with 640 strips. Their compact size, symmetrical sensor position, and DCS4 control unit make the MYTHEN2 series suitable for any diffractometer geometry — from portable instruments to large systems.
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Compact Photon Counting X-Ray Detector
HyPix-3000
Rigaku’s HyPix-3000 is a next-generation two-dimensional semiconductor detector designed specifically to meet the needs of the home lab diffractionist. One of the HyPix-3000’s unique features is its large active area of approximately 3000 mm² with a small pixel size of 100 μm², resulting in a detector with high spatial resolution. In addition, the HyPix-3000 is a single photon counting X-ray detector with a high count rate of greater than 10⁶ cps/pixel, a fast readout speed and essentially no noise.
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Lasers And LEDs
AGILE features a broadband spectral output from <400 nm to >2000 nm and pulse repetition rates from 10 kHz to 1 MHz, making it the ideal light source for the majority of fluorescence lifetime applications. Using the Time-Correlated Single Photon Counting (TCSPC) technique, fluorescence lifetimes from a few picoseconds to microseconds can be accurately resolved. It is also compatible with Multi-Channel Scaling (MCS) mode for lifetimes up to 10 μs.
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Fluorescence Lifetime Spectrometer
S-FL
The technique of Time Correlated Single Photon Counting (TCSPC) has been developed and introduced more then 25 years ago. The technique is now widely accepted to be the most sensitive fluorescence detection technique with the inherent temporal resolution required for fluorescence decays.
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Photon Sensors
Nordson Measurement & Control Solutions
Electrode Coat Weight Gauging of Anode and Cathode for Lithium Ion Batteries
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Avalanche Photodiodes
These avalanche photodiodes (APDs) are silicon photodiodes with an internal gain mechanism. As with a conventional photodiode, absorption of incident photons creates electron-hole pairs. A high reverse bias voltage creates a strong internal electric field, which accelerates the electrons through the silicon crystal lattice and produces secondary electrons by impact ionization. The resulting electron avalanche can produce gain factors up to several hundred.
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Components for System Integration
Bh offers a wide range of accessories to improve your photon counting experiment such as experimental control modules, optomechanics or implantable fiber probes for in-vivo applications. For PMTs and MCPs we offer different preamplifiers and a variety of routing devices for multi-detector operation. For a perfect SYNC signal, trigger modules and a SYG are available.
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Streak Cameras
Streak camera technology was developed for measuring ultra-fast optical phenomena. OptoScope streak cameras provide temporal resolution down to the Picosecond regime. Additionally, OptoScope systems have high sensitivity allowing single photon detection. Streak cameras are the only instruments that can capture the behavior over time of multiple optical signals. Combined with a spectrometer this allows their application in the field of time resolved spectroscopy.
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TCSPC Lifetime Fluorometer
DeltaFlex
The DeltaFlex time correlated single photon counting (TCSPC) system is one of our Delta series of next generation time correlated single photon counting lifetime instrumentation. The DeltaFlex offers the ultimate in flexibility.
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HiCAM
The HiCAM is a gated intensified high-speed high-sensitivity imaging camera. It has an integrated fiber-optically coupled image intensifier, which offers a unique combination of high speed and sensitivity down to single photon level. Because the HiCAM does not need high intensity light sources, it is suitable for use in low-light level conditions.
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TCSPC Lifetime Kit
DeltaTime
The DeltaTime time correlated single photon counting (TCSPC) lifetime plug-in offers acquisition speed, flexibility, and affordability unavailable in any other multifunctioanl fluorescence solution on the market. DeltaTime seamlessly integrates monochromators, polarizers, and other accessories with the widest array of sources (LEDs, laser diodes, supercontinuum lasers) and detectors (including NIR), providing lifetime coverage from 25ps to 1sec over wavelengths spanning the UV to NIR.
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Underwater Quantum/PAR Sensors
Photosynthetic radiation is essential for the growth of the photosynthetic organisms such as corals. The wavelength range from 400 to 700 nm is PAR (Photosynthetically Active Radiation) or PPFD (Photosynthetic Photon Flux Density). Apogee quantum/PAR sensors are calibrated to measure the number of photons of light across this range.
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Spectral Sensitivity Measurement
It is a device which measures the spectral sensitivity characteristics and quantum efficiency of various solar cells by irradiating solar cells with monochromatic light of constant energy and constant photon without wavelength dependence. We are constantly monitoring irradiation light quantity with our real real time light quantity monitor control system and are not influenced by fluctuation of light source, so it is a well-established control system with excellent measurement stability and measurement reproducibility.
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Single Photon Detector System For Near-Infrared (1.6-2.3 Um Wavelength) Waves With Liquid Helium (LHe) Cryostat
Insight Product Company is proud to offer Single Photon Detector System for Near-Infrared (1.6-2.3 um wavelength) with Liquid Helium (LHe) Cryostat. Insight Product Co. offers superconducting single photon detectors and ultra-low noise registration systems for the near infrared range. All systems operate in continuous mode, no gating required.
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High Purity Germanium (HPGe) Radiation Detectors
Semiconductor based photon radiation detectors have been evolving for over half a century, with ORTEC pioneering commercial availability for a majority of that time. Initial offerings were based around lithium-drifted germanium Ge(Li) and lithium-drifted silicon Si(Li). Ge(Li) was later replaced with more advanced, high purity germanium (HPGe) detectors. ORTEC provides a comprehensive suite of HPGe detector solutions covering an extensive range of energies and for a variety of applications.
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Bare Fiber Aligner
1120
The Photon Kinetics 1120 Bare Fiber Aligner makes it possible to reduce test setup time to seconds, thereby reducing overall testing cost. Just strip the fiber, scribe and break it (or use a more precise fiber cleaver, if desired) and then insert the prepared end into the 1120. In an instant, the fiber is coupled to your OTDR or chromatic dispersion test system with low optical loss and low reflectance. The 1120's compact, ergonomic industrial design is well-suited for low to moderate volume fiber and cable testing applications where automated fiber alignment systems are less economical. It is particularly useful as part of an in-process or finished cable test station employing either the 8000i or 8000 OTDR, and the OASYS.net OTDR Automation Software.
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Scientific CMOS Camera
Prime 95B
The Prime 95B Scientific CMOS camera allows you to overcome many difficult imaging challenges by converting nearly every available photon to useful signal through an incredible 95% Quantum Efficiency by using the first available scientific CMOS sensor with back-side illumination. The result is the most sensitive CMOS camera available for scientific imaging.
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X-Ray Components
Photonis designed the Micro Pore Optics detector to be used in X-Ray imaging applications. Its perfectly square, flat channels are optimized to allow X-Ray and UV photons to be focused or collimated due to the total external reflection at a grazing angle (<2°). Micro Pore Optics are installed on a number of international space missions.
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Photon Magnetic Resonance
Numis Poly
The Numis Poly device is a Magnetic Resonance Sounding (MRS) system for the direct detection of shallow groundwater down to 150 m of depth
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SWIR Cameras
Our SWIR or Short-Wave Infrared imaging covers the wavelength range from 900nm to 1700nm. A large number of applications that are difficult or impossible to perform using visible light are made possible, with great results, using short-wave infrared (SWIR) imaging thus enabling the user to "See Beyond the Visible". SWIR is similar to visible light in that photons are reflected or absorbed by an object, providing the strong contrast needed for higher resolution imaging– unlike thermal images, that rely on radiated photons. At NIT, we offer unique SWIR cameras and sensors, see below for more information on our products.
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Single Photon Counting Module
COUNT® Q
COUNT Q - the single photon counting module for the wavelengths range between 900 and 1600 nm! Wavelength range 900 - 1600 nm Detection efficiency: adjustable up to 20% Dark count rate: typ. 1000 cps
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Photon Doppler Velocimeter - MATRIQ
The Quantifi Photonics Doppler instrument combines the key optical components for Photonic Doppler Velocimetry (PDV) measurements in a compact instrument to enable streamlined high-channel count PDV test setups.
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Testing for Si Solar Cells Using High Performance CCD
EL Imaging Tester
EL Testing for Si Solar Cells using High Performance CCD. The determination of luminescence (photo emissions) in solar cells is an important characterization tool. Typical solar cells often have defects which limit the efficiency or lifetime of a cell. Many of these defects are visualized with Luminescence Imaging. By using this technique, the manufacturing process can be optimized to produce better cells. Luminescence Imaging takes advantage of the radiative inter-band recombination of excited charge carriers in solar cells. The emitted photons can be captured with a sensitive CCD camera to obtain an image of the distribution of the radiative recombination in the cell. This distribution is determined by the local excitation level, allowing the detection of electrical losses, thus mapping the diffusion length of minority carriers as the emitted light is low intensity and in the near infra-red range, the CCD camera has a high sensitivity wavelength from 900 to 1100 nm with little thermal noise. This CCD camera provides excellent resolution of 1024 x 1024 pixels with a large 1μm pixel size, multi-megahertz readout speed, and robust USB 2.0 connectivity. The EL CCD Camera is the ultimate high-performance CCD camera for electroluminescence and photoluminescence imaging for Photovoltaic (PV) Cells and Modules. This camera combines low noise electronics and optimal sensitivity in NIR.
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Single Photon Detector System For Near-Infrared (1.6-2.3 Um Wavelength) Waves With Closed-Cyle Cooling
Single Photon Detector System for Near-Infrared (1.6-2.3 um wavelength) waves with Closed-Cylce (cryogen-free)cooling
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SparkFun Photodetector Breakout
MAX30101 (Qwiic)
The SparkFun Photodetector Breakout is an updated version of the SparkFun Particle Sensor Breakout includes the MAX30101, a highly sensitive optical sensor and successor to the MAX30105 and MAX30102. The MAX30101 Breakout utilizes a photon detector to measure the amount of returning light that is reflected back from the LEDs. This is useful for various applications like particle (i.e. smoke) detection, proximity measurements, and even photoplethysmography. To make it even easier to use this breakout, all communication is enacted exclusively via I2C, utilizing our handy Qwiic system. However, we still have broken out 0.1" spaced pins in case you prefer to use a breadboard.
