Finite-element assembly approach of optical quantum walk networks

Christopher R. Schwarze, David S. Simon, Anthony Manni, A. Ndao, Alexander V. Sergienko
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Abstract

We present a finite-element approach for computing the aggregate scattering matrix of a network of linear coherent scatterers. These might be optical scatterers or more general scattering coins studied in quantum walk theory. While techniques exist for two-dimensional lattices of feed-forward scatterers, the present approach is applicable to any network configuration of any collection of scatterers. Unlike traditional finite-element methods in optics, this method does not directly solve Maxwell's equations; instead it is used to assemble and solve a linear, coupled scattering problem that emerges after Maxwell's equations are abstracted within the scattering matrix method. With this approach, a global unitary is assembled corresponding to one time step of the quantum walk on the network. After applying the relevant boundary conditions to this global matrix, the problem becomes non-unitary, and possesses a steady-state solution which is the output scattering state. We provide an algorithm to obtain this steady-state solution exactly using a matrix inversion, yielding the scattering state without requiring a direct calculation of the eigenspectrum. The approach is then numerically validated on a coupled-cavity interferometer example that possesses a known, closed-form solution. Finally, the method is shown to be a generalization of the Redheffer star product, which describes scatterers on one-dimensional lattices (2-regular graphs) and is often applied to the design of thin-film optics, making the current approach an invaluable tool for the design and validation of high-dimensional phase-reprogrammable optical devices and study of quantum walks on arbitrary graphs.
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光量子漫步网络的有限元组装方法
我们提出了一种有限元方法,用于计算线性相干散射体网络的总散射矩阵。这些散射体可以是光学散射体,也可以是量子行走理论中研究的更一般的散射币。虽然已有针对前馈散射体二维网格的技术,但本方法适用于任何散射体集合的任何网络配置。与光学中的传统有限元方法不同,这种方法并不直接求解麦克斯韦方程,而是在散射矩阵方法中抽象出麦克斯韦方程后,用来组合和求解线性耦合散射问题。通过这种方法,可以组装出一个与网络量子行走的一个时间步相对应的全局单元。在对这个全局矩阵应用相关边界条件后,问题就变成了非单元式,并拥有一个稳态解,即输出散射状态。我们提供了一种算法,可以通过矩阵反演精确地获得该稳态解,从而得到散射态,而无需直接计算特征谱。然后,我们在一个具有已知闭式解的耦合腔干涉仪示例上对该方法进行了数值验证。最后,该方法被证明是雷德赫弗星积的广义化,雷德赫弗星积描述了一维晶格(2-不规则图)上的散射体,经常被应用于薄膜光学的设计,这使得目前的方法成为设计和验证高维相位可编程光学设备以及研究任意图上量子行走的宝贵工具。
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