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Integrated photon pair source for SOI-based quantum optics

机译:基于SOI的量子光学集成的光子对源

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Photon pair sources are an important building block for optics based Quantum Information Processing (QIP) such as Quantum Key Distribution (QKD) and Linear Optics Quantum Computing (LOQC) [1]. Beyond the demand for reliable and cheap photon pair sources for QKD, LOQC also requires interferometers that are mechanically stable and loss-free for which integrated photonics is particularly attractive [2]. In this context, photon pair generation (PPG) has been demonstrated via the third order nonlinear interaction between a silicon straight waveguide (Si-w) and a pulsed beam [3]. Such a source cannot be directly followed by other integrated components as photon pairs would be generated throughout the silicon chip. The solution we propose to suppress the pump beam consists of a Sagnac Loop Interferometer (SLI) in which photon pairs are generated and pump beam destructively interferes with itself, thereby allowing photon pairs to be generated in a localised part of the silicon chip. Furthermore, our study has been performed in a continuous instead of a pulsed regime, thereby avoiding any synchronization between detectors and laser and allowing for much cheaper laser sources. Our experimental setup is presented in Fig. 1. The experiment is performed at different pump power both in the a Si-w and the SLI. Results are presented in Fig. 2. The flux of generated pairs and the Signal-to-noise ratio are limited by the outcoupling loss and detector inefficiency. The photon flux is less than expected because the emitted spectrum is around 8nm (FWHM) broad instead of the expected 70nm. The performance of the SLI is not yet perfect: the pump suppression efficiency decreases with the pump power (from -22dB to -15dB) due to unexpected nonlinear behaviour in the directional coupler that changes the coupling ratio; and the Signal-to-Noise ratio is lower than in the Si-w which might be due to PPG in the broad (800nm) waveguide before the SLI.
机译:光子对源是基于光学的量子信息处理(QIP)的重要构建块,例如量子密钥分布(QKD)和线性光学量子计算(LOQC)[1]。除了对QKD的可靠和便宜的光子对源的需求之外,LOQC还需要干涉仪,该干涉仪是没有机械稳定和损失的,为此综合光子学特别吸引力[2]。在这种情况下,通过硅直波导(Si-W)和脉冲梁之间的三阶非线性相互作用和脉冲梁[3]已经证明了光子对生成(PPG)。这种源不能直接遵循其他集成组件,因为光子对将在整个硅芯片中产生。我们提出抑制泵浦光束的解决方案包括凸隙环路干涉仪(SLI),其中产生光子对并且泵浦束破坏性地干扰,从而允许在硅芯片的局部部分中产生光子对。此外,我们的研究已经以连续的而不是脉冲制度进行,从而避免了检测器和激光之间的任何同步并允许更便宜的激光源。我们的实验设置如图1所示。实验在Si-W和SLI中以不同的泵功率进行。结果如图2所示。产生对的磁通量和信噪比受到外耦合损耗和检测器效率效率的限制。光子通量小于预期,因为发射的光谱是宽约8nm(fwhm)宽而不是预期的70nm。 SLI的性能尚不完美:由于在改变耦合率的定向耦合器中的意外非线性行为,泵抑制效率随泵浦电源(从-22db到-15db)减小;并且信噪比低于Si-W中,这可能是由于SLI之前的宽(800nm)波导中的ppg。

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