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Home > Products > Light Test and Measurement > Detectors > SPM Series High Gain Avalanche Photodiode Detectors

SPM Series High Gain Avalanche Photodiode Detectors
SPM Series High Gain Avalanche Photodiode Detectors

  • Compact, rugged and stable detector supplied with integrated power supply and TE cooler
  • High gain (106)
  • Low bias voltages (30V)
  • Fast rise time (<5ns)
  • Low dark count rate (<1MHz)
  • Large area up to 9mm2
Applications
  • Fluorescence lifetime measurements
  • Biological sensors
  • Scanning microarrays
  • DNA biochips/sequencing
  • Proteomics/Protein Biochips
  • Point-of-use biological agent detection
  • Confocal microscopy
  • Nuclear medicine
  • Environmental monitoring
  • Nuclear radiation detection
  • Homeland security
  • High energy physics
  • Flow cytometry
  • Capillary electrophoresis
  • Range finding

Product Description Product Detail Specifications Drawings Downloads Catalog PDF
Product Description
Whether your application is a large area radiation detection, a benchtop instrument or a higher tier laboratory analysis instrument, the SPM Series will provide significant benefit over existing detector platforms.
The SPM Series High Gain Avalanche Photodiodes are the first solid state alternative to the long established Photomultiplier Tube (PMT). These devices combine the high gain (106) and high quantum efficiency of the PMT with the well appreciated benefits of silicon including size, low operating voltage, robustness, reliability, magnetic field insensitivity, tolerance of excess/ambient light and suitability for miniaturization. In addition, this novel design has a high signal to noise ratio and a very fast pulse response.
The detector consists of an array of Geiger mode Avalanche Photodiodes (APDs), each individually coupled to integrated quench electronics, and is a type of detector commonly referred to as a Silicon Photomultiplier (SPM). Geiger mode APDs have extremely high internal amplification that allows single photon sensitivity at room temperature. The output of a Geiger mode APD is an identical, fixed charge or current pulse for each single photon detected. By connecting an array of Geiger mode APDs in parallel, the summed output becomes proportional to the number of Geiger mode pulses and hence ...


Ordering Information
 Quantity Model Description Price
  SPM1Q-T SPM: Silicon Photomultiplier (High Gain APD), 1mm x 1mm Detector QE Optimized, Transimpedance Amplifier) 
  SPM1D-T SPM: Silicon Photomultiplier (High Gain APD), 1mm x 1mm Detector DR Optimized, Transimpedance Amplifier) 
  SPM1Q-P SPM: Silicon Photomultiplier (High Gain APD), 1mm x 1mm Detector QE Optimized, Pulse Amplifier) 
  SPM1D-P SPM: Silicon Photomultiplier (High Gain APD), 1mm x 1mm Detector DR Optimized, Pulse Amplifier) 
  SPM3Q-T SPM: Silicon Photomultiplier (High Gain APD), 3mm x 3mm Detector QE Optimized, Transimpedance Amplifier) 
  SPM3D-T SPM: Silicon Photomultiplier (High Gain APD), 3mm x 3mm Detector DR Optimized, Transimpedance Amplifier) 
  SPM3Q-P SPM: Silicon Photomultiplier (High Gain APD), 3mm x 3mm Detector QE Optimized, Pulse Amplifier) 
  SPM3D-P SPM: Silicon Photomultiplier (High Gain APD), 3mm x 3mm Detector DR Optimized, Pulse Amplifier) 
  SPM-CM C Mount Adaptor 
  SPM-F FC Adapter for Fiber Coupling 

APD = Avalanche Photodiode

QE = Quantum Efficiency

DR = Dynamic Range
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