Undetected photon interference measurements on a silicon chip

Chiara Michelini, S. Signorini, V. Pruneri, Lorenzo Pavesi
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Abstract

Interference measurements with undetected photons employ entangled photon pairs in order to overcome classical limitations in measurement sensitivity. With the undetected photon technique, one photon (signal) interacts with an object, and the signature of the interaction is stored in its entangled counterpart (idler): the interacting photon remains undetected, while the detection is performed on the photon that did not interact with the object. While the signal photon can be chosen in any spectral region suitable for the interaction, the idler photon is generated in a spectral region where detectors are efficient, scalable, and cheap. To date, the configurations proposed are in bulk setups. In this work, we propose a novel configuration on an integrated device, with the advantages of the reduced dimension, the lower cost and the robustness to alignment. In our experiment, we pumped a silicon-on-silica integrated circuit with a classical beam at a wavelength of 1.568 μm. Via intermodal spontaneous four-wave mixing, we generated highly non-degenerate time-energy entangled signal and idler photons at 1.99 μm and 1.29 μm, respectively. As we have integrated two identical sources of entangled photons in series, the photon pairs generated in the two sources are indistinguishable, and controlling the phase of the pump beam and the phase of the signal photons after the first nonlinear source, we observed interference patterns with 24% maximum visibility in the idler photon counts. We successfully measured the dephasing induced on the signal photons by measuring only the idler ones.
在硅片上未被探测到的光子干涉测量
未探测光子的干涉测量采用纠缠光子对,以克服测量灵敏度的经典限制。在未检测到的光子技术中,一个光子(信号)与一个物体相互作用,而相互作用的特征被存储在其纠缠的对应(空闲)中:相互作用的光子仍然未被检测到,而检测是在未与物体相互作用的光子上进行的。虽然信号光子可以选择在任何适合相互作用的光谱区域,但空闲光子是在探测器高效、可扩展和廉价的光谱区域产生的。到目前为止,建议的配置是批量设置。在这项工作中,我们提出了一种新的集成器件结构,具有减小尺寸,降低成本和对准鲁棒性的优点。在我们的实验中,我们用波长为1.568 μm的经典光束泵浦硅对硅集成电路。通过多模态自发四波混频,我们分别在1.99 μm和1.29 μm处产生了高度非简并的时间-能量纠缠信号和空闲光子。由于我们将两个相同的纠缠光子源串联在一起,两个源中产生的光子对是不可区分的,并且在第一个非线性源之后控制泵浦光束的相位和信号光子的相位,我们观察到在空闲光子计数中具有24%最大可见度的干涉图案。我们仅通过测量空闲光子就成功地测量了信号光子所引起的失相。
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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