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基于InGaAs/InP低噪声GHz单光子探测器研究(特邀)
引用本文:龙耀强,单晓,武文,梁焰. 基于InGaAs/InP低噪声GHz单光子探测器研究(特邀)[J]. 红外与激光工程, 2023, 52(3): 20220901-1-20220901-8. DOI: 10.3788/IRLA20220901
作者姓名:龙耀强  单晓  武文  梁焰
作者单位:上海理工大学 光电信息与计算机工程学院,上海 200093
基金项目:国家重点研发计划(2021YFB2801100);国家自然科学基金(62175152,61927813)
摘    要:InGaAs/InP雪崩光电二极管(APD)体积小、功耗低、响应速度快,被广泛应用于近红外单光子检测。文中分析了APD雪崩及噪声信号的频谱分布特征,提出了正弦门控结合低通滤波级联方案,噪声抑制比超过40 dB,实现了1~2 GHz高性能探测。当工作速率为1.5 GHz,探测效率设置为20.0%时,后脉冲概率为6.6%,暗计数率仅为6.7×10-7/gate。此外,集成了APD高速门控产生及延时调节模块,温度反馈稳定控制模块,实现了单光子探测器12 h稳定运行,计数标准差仅为1.0%。最后,为了更完整的描述探测器的量子特征,引入量子探测器层析技术进行标定,重新构建了其正值算符测度矩阵以及对应的Wigner函数,为其在量子通信、量子计算等量子信息技术的应用中提供支撑。

关 键 词:单光子探测器  雪崩光电二极管  低通滤波  量子层析
收稿时间:2022-12-27

Low-noise GHz InGaAs/InP single-photon detector (invited)
Affiliation:School of Optical-Electrical and Computer Engineering, University of Shanghai for Science and Technology, Shanghai 200093, China
Abstract:  Objective  With the development of quantum information science, laser radar and deep space detection, the traditional linear photoelectric detection technology has been unable to meet the needs of sensitive optical signal detection. The single-photon detection technology has gradually become an important research in the fields of weak light detection. InGaAs/InP avalanche photodiodes (APDs) are widely used in near-infrared single-photon detection due to the small size, low power consumption and fast response. The detection rate of most commercial InGaAs/InP detectors is at the level of 100 MHz, which cannot meet the application requirements for high counting rate. Meanwhile, low noise of the APD will bring smaller false counts to the system and further improve the performance. Therefore, a low-noise InGaAs/InP single-photon detector operating at the repetition frequency of GHz was demonstrated. Furthermore, the whole detector is evaluated with the quantum detector tomography technology, providing support for its application in quantum information technology such as quantum communication and quantum computation.   Methods  In order to determine the detection frequency of gating signals, the response bandwidth of the APD is analyzed in the linear mode, and the bandwidth range is calculated to be 1-2 GHz. The spectral distribution characteristics of APD avalanche and noise signals are analyzed in the Geiger mode. It could be figured out that the noise is mainly distributed in the gating frequency and its harmonic frequencies, while the avalanche signal is mainly distributed below 1 GHz. Therefore, a cascade scheme of sine wave gating combined with low-pass filtering is proposed (Fig.3). The detector comprises high-speed gate generation and delay regulation module, temperature feedback control module, etc. Sine wave gating could be precisely controlled from many parameters which include frequency, amplitude, delay in a wide range. Feedback is added in the temperature control module to improve the stability of the detector. In addition, quantum detector tomography (Fig.2) is introduced to calibrate the detector, which is regarded as a "dark box". The positive operator-value measuring matrix can fully characterize the detector, which is obtained from input states and output results. The Wigner function is employed to describe whether the detector has quantum properties at high input photons.   Results and Discussions   Sine wave gating combined with low-pass filtering is designed in the system, and signal-to-noise ratio is over 40 dB. The relationship between the detection efficiency and the afterpulse probability at the frequencies of 1-2 GHz is recorded. When the working rate is 1.5 GHz and the detection efficiency is set to be 20.0%, the afterpulse probability is 6.6% with the dark count rate of only 6.7×10?7 per gate (Fig.4). At constant detection efficiency of 20.0%, the DC bias voltage of the APD increases with temperature, showing a linear trend. While the afterpulse probability decreases, showing a contracting trend. The dark count rate degrades with the decrease of temperature and the trend is reversed at ?30 ℃ (Fig.5), which might be related to high afterpulse or the intrinsic defection of APD. During the 12-hour test period, the detector performs perfectly stable and the variance of detection efficiency is 1% (Fig.8). Quantum detector tomography technology is employed to verify that high background noise does not affect the quantum properties (Fig.7).   Conclusions  A GHz low noise InGaAs/InP detector is designed, and its detection efficiency, false count, saturation count rate and stability are explored. Based on the analysis of the response bandwidth of APD, a cascade scheme of sine wave gating combined with low-pass filtering is determined, realizing a low noise single photon detection below 2 GHz. In addition, quantum detector tomography technology is employed to calibrate the detector and verify its quantum properties. The structure of the detection technology is simple and the detector can run stably in the long term, which provides strong support for the practical application of single photon detector in deep space communication, laser mapping, optical time domain reflection and other fields.
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