Single Photon Communication with Avalanche Diodes and the General Basics of Photon Counting

Boldizsár Kurilla
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Abstract

Single photon communication (SPC) already exists in several applications in laboratory and even outdoor conditions. In the field of quantum cryptography SPC experiments are part of military applications too. There are several methods to detect every single impacting photon in such an experiment. Mostly photomultiplier tubes (PMT) are used. In some cases single photon avalanche diodes (SPAD) are more suitable for photon detection. Both the SPADs and PMTs have advantages and disadvantages. Usually PMTs have much larger detection areas than SPADs, but most of the PMTs detection efficiency peaks at 400 nm wavelength compared to the SPADs, where it peaks at 600–700 nm wavelength. For long distance laser measurements the higher wavelength is more suitable due to the Rayleigh scattering, but the detection hole of SPAD is very tight, which is why it is really hard to target the laser punctually without an optical gyroscope.
雪崩二极管的单光子通信和光子计数的一般基础
单光子通信(SPC)已经在实验室甚至室外条件下得到了广泛应用。在量子密码学领域,SPC实验也是军事应用的一部分。在这样的实验中,有几种方法可以检测到每个单个的冲击光子。主要使用光电倍增管(PMT)。在某些情况下,单光子雪崩二极管(SPAD)更适合于光子探测。spad和pmt都有各自的优缺点。通常,pmt的检测面积比spad大得多,但大多数pmt的检测效率峰值在400 nm波长,而spad的检测效率峰值在600-700 nm波长。对于长距离激光测量,由于瑞利散射,波长越高越适合,但SPAD的探测孔非常紧,这就是为什么没有光学陀螺仪很难及时瞄准激光。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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