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Single Photon Counting Modules
Single photon counting modules. So-called single photon counting modules are used to count single photons. These photon counters, sold under the brand name COUNT®, offer phenomenally low dark count rates with the best low noise characteristics.
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Single Photon Detector System For Near-Infrared (0.7 - 1.3 Um Wavelength)
Single Photon Detector System for Near-Infrared (0.7 - 1.3 um wavelength) waves with Closed-Cylce (cryogen-free)cooling
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Multipurpose X-Ray Diffractometer with Built-In Intelligent Guidance
SmartLab SE
The SmartLab® SE is a highly versatile multipurpose X-ray diffractometer with built-in intelligent guidance. It offers continued refinement of the original ease of use features that enabled the original SmartLab to receive the R&D 100 Award in 2006: automatic alignment, component recognition, cross beam optics and advanced photon counting hybrid pixel array detectors (HPAD).
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Instrument Software for SPC- and DPC Modules
SPCM
*Multifunctional 64 bit Data Acquisition Software*Recording of Multi-Dimensional TCSPC Results and Time-Tag Data*Control of Multi-Dimensional Recording Features*Configurable User Interface*Acquisition of Decay Curves, FCS, MCS Traces, FLIM and PLIM Images*Online Calculation and Display of FLIM, PLIM, FCS, PCH, MCS Traces and Fit of FCS Curves*Different Operation Modes Available*Measurement Control of Up to 4 Modules*Configurable for Different Instrument Configurations*Accumulation and Autosave Functions*Integrated Scanner Control*Saving, Loading and Conversion of Photon Distributions, Images and Time-Tag Data*Saving and Loading of Results and System Parameters*Integrated Control of Ti:Sa Lasers*Integrated Control of Motor Stages
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PIN Photodiode
PIN photodiode is a kind of photo detector, it can convert optical signals into electrical signals.This technology was invented in the latest of 1950's. There are three regions in this type of diode. There is a p-region an intrinsic region and an n-region. The p-region and n-region are comparatively heavily doped than the p-region and n-region of usual p-n diodes. The width of the intrinsic region should be larger than the space charge width of a normal p-n junction. The PIN photo diode operates with an applied reverse bias voltage and when the reverse bias is applied, the space charge region must cover the intrinsic region completely. Electron hole pairs are generated in the space charge region by photon absorption. The switching speed of frequency response of photo diode is inversely proportional to the life time. The switching speed can be enhanced by a small minority carrier lifetime. For the photo detector applications where the speed of response is important, the depletion region width should be made as large as possible for small minority carrier lifetime as a result the switch speed also increases.
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Underwater Quantum Sensor
LI-192
The LI-192 Underwater Quantum Sensor measures PAR from all angles in one hemisphere. The LI-192 works in air or underwater at depths up to 560 meters. The measurements are cosine corrected and typically expressed as Photosynthetic Photon Flux Density (PPFD). For simultaneous measurements of downwelling and upwelling PAR, two sensors can be mounted on the 2009S Lowering Frame.
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Solar Simulators
Sun 2000 Class A
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. A digital shutter timer allowing both manual and external control is included with every unit.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.
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Proximity Sensors
Unlike other proximity sensors that use simple IR (Infra-Red) technology, which only measure signal strength and can be affected by the object’s reflectivity, FlightSense™ sensors directly measure distance to the object based on the time for emitted photons to be reflected, enabling accurate distance ranging regardless of the object’s surface characteristics.
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Raman Spectroscopy
Raman is a spectroscopic technique that uses laser light to interact with molecular excitations and determine what a substance or element is composed of. It relies upon the inelastic scattering of photons which produces a weak signal, making the collection of information challenging particularly when the substance to be measured is at distance or can only be given short exposure times. Our Raman spectrometers are particularly effective at making Raman measurements due to their configuration which delivers a higher throughput/etendue than standard instruments.
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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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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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Avalanche Photodiodes
Excelitas offers Avalanche Photodiodes (APDs) on both Silicon (Si) and InGaAs materials. Si APDs cover the spectral range of 400 nm to 1100 nm and the InGaAs APDs cover 950 nm to 1550 nm. An Avalanche Photodiode (APD) provides higher sensitivity than a standard photodiode and is for extreme low-level light (LLL) detection and photon counting.
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Random Number Generation
Quantis is a family of hardware random number generators (RNG) which exploit elementary quantum optical processes as a source of true randomness (cf. Wikipedia: physical phenomena with quantum random properties). Photons (light particles) are sent, one by one, onto a semi-transparent mirror and detected. The exclusive events (reflection or transmission) are associated to “0” or “1” bit values. Such quantum processes provide instantaneous and inexhaustible entropy.
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Preclinical Imaging Modalities and Solutions
Bruker offers advanced preclinical imaging solutions for a broad spectrum of application fields, such as oncology, neurology, cardiology, inflammation, infectious diseases, cancer research, functional and anatomical neuroimaging, orthopedics, cardiac imaging and stroke models. Our range of techniques includes MRI (Magnetic Resonance Imaging) , PET (Positron Emission Tomography), SPECT (Single Photon Emission Computed Tomography) micro-CT (Micro Computed Tomography), optical imaging and magnetic particle (MPI) imaging.
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XRT Source Brighthawk
The BRIGHTHAWK NT100 is a performance-leading microfocus X-ray tube comprising proprietary technology to achieve a high brightness output. The tube consists of a LaB6 crystal source for generation of the electron beam, a magnetic beam steering system, and a tungsten target for X-ray photon emission. The components are mounted in a precision-engineering housing and held at ultra-low vacuum levels for long-life performance. Following on from the successful 3rd generation tube, this 4th generation of tube across a wide energy range from 30 kV to 160 kV is highly configurable through a software interface to the internal control board, which is connected via an optical interface (through an Ethernet converter).
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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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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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Photon Sensors
Nordson Measurement & Control Solutions
Electrode Coat Weight Gauging of Anode and Cathode for Lithium Ion Batteries
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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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Intensified Cameras
Excelitas offers a broad range of single to multi-channel image intensified cameras through our renowned pco.dicam series. With extreme short exposure times down to 2.5 ns, our pco.dicam cameras offer the ability to precisely address ultra-fast processes far beyond the capabilities of any other camera type. Featuring state-of-the art scientific CMOS sensor technology, our pco.dicam intensified cameras combine high resolution, fast frame repetition rates, 16-bit dynamic range and extreme sensitivity for efficient single photon detection.
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Photon Magnetic Resonance
Numis Lite
The Numis lite device is a Magnetic Resonance Sounding (MRS) system for the direct detection of shallow groundwater down to 50 m of depth.
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Photosynthetically Active Radiation Probe
LPPAR01
The LPPAR01 probe measures the ratio between the number of photons that strike a surfacein one second, in the 400 nm…700 nm spectral range and the surface area (m2). This quantity is defined as PAR: Photosynthetically Active Radiation.
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Fluorescence Lifetime Systems
TCSPC, short for time-correlated single photon counting, refers to a powerful analysis method used especially in life sciences and fundamental physics. This technique is used to perform hyper-accurate fluorescence and phosphorescence lifetime measurements. As technology leader in equipment for multidimensional single photon counting, Becker & Hickl has been offering a wide range of high-efficiency TCSPC systems since 1993.
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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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Photon Counting Cameras
Photek photon-counting camera systems are unique as they provide the ability to capture and integrate an image in real time. These systems are ideal for extremely low photon emission applications such as bio-luminescence, chemi-luminescence and weak fluorescence. The ability to accurately analyze transient events is a key feature of this product. The length of time that the image can be integrated is limited only by disc space, and allows the user to fully capture real-time events. X, Y and time co-ordinates for post acquisition analysis is also recorded. X-ray and vacuum imaging camera options are also available.
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Auto-Correlator
FR-103TPM
The FR-103TPM is a high resolution, easy-to-use Autocorrelator for Two Photon Microscopy. It can be introduced into the beam path without disturbing the optical alignment, with the detector package replacing the sample.
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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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Detectors
Designed and manufactured by Becker & Hickl - bh offers a wide range of detector types as photomultiplier tubes (PMC), hybrid photo detectors (HPM), single-photon avalanche diodes (SPAD) as well as multi-channel- and multi-spectral detectors. The detection range covers the wavelengths from UV to the NIR and time resolutions spanning from tens of ps to hundreds of ps suitable for anti-bunching, FCS, FLIM, PLIM and other applications. bh guarantee that their TCSPC modules work with any photon counting detector and reach the fastest possible IRF width.Choose your detection now:
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Electron Multipliers
Electron multipliers are mainly used as positive/negative ion detectors. They are also useful for detecting and measuring vacuum UV rays and soft X-rays. Hamamatsu electron multipliers have a high gain (multiplication factor) yet low dark current, allowingoperation in photon counting mode to detect and measure extremely small incoming particles and their energy. This means our Hamamatsu electron multipliers are ideal for electron spectroscopy and vacuum UV spectroscopy such as ESCA (electron spectroscopy for chemical analysis) and Auger electron spectroscopy as well as mass spectroscopy and field-ion microscopy.
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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.
