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Laser Ranging And Lidar APD Photoreceivers

 High-gain, Low-noise Photodetector
 Wide Spectral Response
 High Bandwidth
 Low Noise Equivalent Input (NEI)
 Large Total Dynamic Range
 User-programmable
 Easy to Operate
 Four Factory-calibrated Modes for
Temperature-compensated Operation
 Low System Power Consumption
 Long Lifetime
 Robust
 Flexible Integration

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The GD series of laser-ranging photoreceivers—which integrates  high-performance InGaAs avalanche photodiodes  (APDs), custom-designed CMOS application-specific integrated  circuits (ASICs), high-voltage APD bias circuits, and programmable  processing circuits—provides flexible system integration and reliable  performance, all in a small TO-8 package.  To accommodate new applications and changing operating  conditions, an embedded microcontroller allows quick configuration  of the photoreceiver and optimization of performance as a function  of ambient temperature—without using thermoelectric cooling.  Factory-calibrated settings automatically configure the detector for  one of several modes programmed into the memory of each  photoreceiver. For each operating temperature, these modes  include: constant gain, optimal sensitivity, optimal noise equivalent  input (NEI), and constant responsivity.  To achieve the desired pulse-detection probability and false-alarm  rate (FAR), the threshold voltage of the detector can be manually  adjusted. To reduce false alarms caused by scattering, the threshold  can be adjusted as a function of laser flight time using the timevariable threshold (TVT).  The photoreceiver outputs a differential digital signal for both the rising  edge and the falling edge of a pulse. This allows time-over-threshold  (TOT) correction to be used where range-walk errors would otherwise  result from variations in pulse amplitude. The analog output allows  signals to be digitized and pulse processing to be performed.  A range of APD diameters and immersion lens options are available.  

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