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Detectors
Detectors are used to measure the illumination of a light source for a number of optical or spectrometry applications. Detectors consist of arrays of photodiodes or photodetectors that transmit electrical current when excited by collision from photons. Detectors enable the measurement of important light characteristics that are not conveniently acquired in other ways. A selection of photodiodes is also available with linked amplifier capabilities for easier, more precise measurement capacities.Detectors
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Electron Multiplying CCD ("EMCCD") Cameras
Evolve Series
The Evolve® is a high-resolution, back-illuminated EMCCD providing high sensitivity for the lowest light applications.With proprietary Teledyne technology throughout, the Evolve provides a new standard in EMCCD performance and reliability. For single molecule imaging, TIRF microscopy, and more, achieve the best imaging performance when every photon counts.
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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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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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PAR Quantum Radiometric Probe
LP471PAR02
Quantum-radiometric probe for measuring the PHOTONS FLOW in the chlorophyll field PAR (photosynthetically Active Radiation 400…700 nm), μmol m-²s-¹ measure, opaline quartz diffuser for cosine correction.
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PAR Quantum Radiometric Probe
LP471PAR
Quantum-radiometric probe for measuring the PHOTONS FLOW in the chlorophyll field PAR (photosynthetically Active Radiation 400nm…700 nm), μmol m-²s-¹ measure, cosine correction diffuser.
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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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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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Photoreaction Evaluation System
Lightway (PQY-01)
This system can measure the number of photons absorbed, which is necessary for calculating the quantum yield of photoreactions.
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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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Radiometric Probe for Photons Flow
LPPAR03… Series
The probe LPPAR03 measures the ratio between the number of photons that strike a surface in one second, in the 400 nm…700 nm spectral range and the surface area (m²). This quantity is defined as PAR: Photo-synthetically Active Radiation.
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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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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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SHORT PULSE LASER SOURCE
id300 SERIES
The id300 short-pulse laser source is an externally-triggered optical source that generates sub-nanosecond laser pulses. Used in combination with a variable optical attenuator, this source cost-effectively approximates a single photon source.
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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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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 Counting Modules
SPD_A_VIS
The SPD_A_VIS from AUREA Technology is the "best-in-class" high-performance and easy-to-use single photon counting modules engineered for the most demanding low-level-of-light [400 nm - 1060 nm] applications. The SPD_A_VIS can be used in continuous mode (free-running) or in gated-mode.
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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 and a high detection efficiency.
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Spectrophotometers
The PHOTON RT UV-VIS-MWIR research spectrophotometers from EssentOptics are convenient and reliable instruments for a broad range of optical measurement applications. You''''ll always enjoy working with them, trusting their functionality and accuracy.The PHOTON RT UV-VIS-MWIR Universal Scanning Spectrophotometers is a powerful multi-purpose instruments designed for coaters. It offeres incomparably greater advantages when compared with the traditional tools offering unattended measurement of optical thin film coatings including variable angle and polarization-dependent measurements without any attachements.
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SWIR Camera with 85% QE, Low Noise, and over 10 Minute Exposure Times
NIRvana® 640
Teledyne Princeton Instruments
The NIRvana® 640 offers incredible sensitivity with greater than >85% Quantum Efficiency between 950 nm and 1500 nm, ensuring you collect every photon you can.The biggest barrier to low light SWIR imaging is dark current. The NIRvana® 640 offers incredible low dark current – only 40e-/p/s, enabling longer exposures for faint samples.
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Time-Correlated Single Photon Counting Module
LYNXEA_VIS
The LynXea_VIS from AUREA Technology is a stand-alone [400-1060 nm] Time Correlated Single Photon Counting TCSPC module, which fully integrates the Time to Digital Converter and the best single photon avalanche detection (SPAD) counting technologies within the same box. As a matter of fact, TCSPC measurements are now available without assembling multiple boxes!
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Twin Photon Source at Telecom Wavelengths
AUREA Technology offers the first worldwide high-brightness stand-alone Entangled Photon Pair Source at telecom wavelengths, ideal for quantum information technologies. The TPS photon-pair source series are high-performance, compact and easy-to-use self-contained twin photon source. With only 5mW of pump power, it performs a spectral brightness of more than 100,000 photons/s/pm!
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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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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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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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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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Hybrid Picosecond Photon Detectors
HPPD Series
technology.The HPPD is our latest development in TCSPC detector technology that combines the benefits of conventional PMT design (wide spectral response and large active area)with the advantages of solid state APD technology (good detection efficiency, negligible after-pulsing and exceptional temporal resolution). Hybrid detectors are becoming thefirst choice for FLIM and short lifetime determination.
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Analysis Software for FCS and cross-FCS
Burst-Analyzer
*FCS Fit with User-Defined Model Functions*Identification of Single-Molecule Photon Bursts in Parameter-Tag Data*Analysis of Fluorescence Intensity and Lifetime within Photon Bursts*One- and Two-Dimensional Histograms of Burst Parameters*Filtered Histograms of Burst Parameters*Discrimination of Different Fluorescent Species or FRET States*Determination of FRET Efficiencies*Exclusion of Artifacts in Intensity Traces
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Analysis Software for FLIM, PLIM
SPCImage
*Analysis of Single-Decay, FLIM and PLIM Data*Analysis by Iterative Convolution and Fit Procedure or by First Moment of Photon Distribution*Calculations of Decay Parameters and Lifetimes by Various Decay Models*Calculation of FRET Efficiencies*Display of Lifetime and FRET Images*Display of Lifetimes, Amplitudes, Intensities or Ratios*Export of Lifetime Data and Images
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AOI Programming Software
ProntoAOI
ProntoAOI used by electronics manufacturers will quickly program your Automatic Optical Inspection (AOI) machines. Program most popular AOI Equipment such as YES Tech, Mirtec, Orbotech, Agilent, Omron, CyberOptics, Viscom, Quad, Machine Vision Products (MVP), ViTechnology, Landrex Technologies, Christopher Associates / Marantz, Photon Dynamics, Camtek, etc.
