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Measurement System of Correlation Functions of Microwave Single Photon Source in Real Time

机译:实时微波单光子源的相关函数测量系统

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Several quantum setups, such as quantum key distribution networks~([1]) and quantum simulators (e.g. boson sampling), by their design rely on single photon sources (SPSs). These quantum setups were demonstrated to operate in optical frequency domain. However, following the steady advances in circuit quantum electrodynamics, a proposal has been made recently~([21) to demonstrate boson sampling with microwave photons. This in turn requires the development of reliable microwave SPS. It's one of the most important characteristics are the first-order and the second-order correlation functions g_1 and g_2. The measurement technique of g_1 and g_2 is significantly different from that in the optical domain [3],[4] because of the current unavailability of microwave single-photon detectors. In particular, due to high levels of noise present in the system a substantial amount of statistics in needed to be acquired. This work presents a platform for measurement of g_1 and g_2 that processes the incoming data in real time, maximizing the efficiency of data acquisition. The use of field-programmable gate array (FPGA) electronics, common in similar experiments~([3]) but complex in programming, is avoided; instead, the calculations are performed on a standard desktop computer. The platform is used to perform the measurements of the first-order and the second-order correlation functions of the microwave SPS.
机译:几个量子设置,例如量子密钥分配网络〜([1])和Quantum模拟器(例如,Boson采样),其设计依赖于单光子源(SPSS)。这些量子设置被证明在光学频域中运行。然而,在电路量子电动动力学的稳定前进之后,最近已经进行了提案〜([21)用微波光子展示玻色子采样。这反过来需要开发可靠的微波SP。它是最重要的特征之一是一阶和二阶相关函数G_1和G_2。由于微波单光子探测器的电流不可用,G_1和G_2的测量技术与光学域[3],[4]中的测量技术显着不同。特别地,由于系统中存在的高水平噪声,需要获得大量统计数据。这项工作介绍了用于测量G_1和G_2的平台,该平台实时处理传入数据,最大化数据采集效率。使用现场可编程门阵列(FPGA)电子器件,在类似实验中常见的〜([3]),但在编程中复杂;相反,计算在标准桌面计算机上执行。该平台用于执行微波SPS的一阶和二阶相关函数的测量。

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