首页> 外文会议>Device Research Conference >Low Dark Count Rate and High Single Photon Detection Efficiency Avalanche Photodiode in Geiger-mode Operation
【24h】

Low Dark Count Rate and High Single Photon Detection Efficiency Avalanche Photodiode in Geiger-mode Operation

机译:低暗计数率和高单光子检测效率雪崩光电二极管在地冰模式操作

获取原文

摘要

Recently, single photon avalanche detectors (SPADs) have been the subject of numerous research programs due to the emergence of applications such as, quantum cryptography, time resolved spectroscopy, three-dimensional imaging, and optical time domain reflectometry (OTDR). Silicon (Si) avalanche photodiodes (APDs) operated in Geiger-mode achieve very high detection efficiency and low dark count rate. However the bandgap of Si limits their operating wavelength to λ < 1.1μm. For longer wavelength operation, a great deal of research has been done on In{sub}0.53Ga{sub}0.47As/InP-based SACM (Separate-Absorption-Charge Multiplication) APDs as single-photon counters. Most of these studies have used commercially available APDs that were developed for fiber optic transmission. In this paper we report In{sub}0.53Ga{sub}0.47As/InP SPADs designed for low dark current that achieve record dark-count-rate/detection-efficiency performance. The SPAD structure is a 40μm-diameter planar In{sub}0.53Ga{sub}0.47As/InP-based SACM (Separate-Absorption-Charge Multiplication) APDs grown by MOCVD. The breakdown voltages at 297K and 200K were 62.3V and 51.6V, respectively (Fig. 1). The dark current at 95% of the breakdown voltage was 0.18nA and 0.15pA at 297K and 200K, respectively. Such low dark current is an indication of good crystal quality. Geiger-mode operation was characterized using pulse quenching. The SPAD was biased ~0.6V below the breakdown voltage and a 4ns voltage pulse was superimposed through a 30nF capacitor. The repetition rate was 10kHz. A pulsed laser source and a photon counter were synchronized with the voltage pulse. The pulsed laser diode produced optical pulses with width of 400ps at 1310nm. The optical source was attenuated to 0.1 photon per bias gate by a calibrated variable optical attenuator.
机译:最近,由于诸如量子密码,时间分辨的光谱,三维成像和光学时域反射(OTDR)的应用,单个光子雪崩探测器(SPAD)是众多研究程序的主题。硅(SI)在冰叶模式下操作的硅(SI)雪崩光电二极管(APDS)可实现非常高的检测效率和低暗计数率。然而,Si的带隙将其工作波长限制为λ<1.1μm。对于较长的波长操作,在{Sub} 0.53Ga {Sub} 0.47AS / InP的SACM(单独吸收 - 电荷乘法)APDS中已经完成了大量的研究作为单光子计数器。这些研究中的大多数已经使用了用于光纤传输的商业上可用的APD。在本文中,我们在{sub} 0.53ga {sub} 0.47AS / INP SPAD中,设计用于低暗电流,实现历史记录暗计数/检测效率性能。 SPAD结构是由MOCVD生长的{Sub} 0.53gA {亚} 0.47AS / INP的SACM(单独吸收 - 电荷乘法)APDS中的40μm直径的平面。 297k和200k的击穿电压分别为62.3V和51.6V(图1)。 95%的击穿电压的暗电流分别为0.18纳,分别为297k和200k。这种低暗电流是良好的晶体质量的指示。使用脉冲淬火的特征在特征。将其偏置在击穿电压以下〜0.6V,通过30nf电容叠加4ns电压脉冲。重复率为10kHz。脉冲激光源和光子计数器与电压脉冲同步。脉冲激光二极管在1310nm处产生宽度为40ps的光脉冲。通过校准可变光学衰减器将光源衰减至每偏置门0.1光子。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号