时变耦合的盲量子源分离与过程层析成像系统

Y. Deville, A. Deville
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引用次数: 2

摘要

经典的盲源分离(BSS)方法,即非量子盲源分离(BSS)方法,只使用由这些源信号通过混合变换传输得到的混合信号来估计未知源信号,这些信号通常具有未知的参数值。我们开发了量子版本的BSS(称为BQSS),并将其扩展到未知混合/耦合参数的盲估计,从而实现了盲量子过程层析成像(BQPT)。在这些研究中,混合参数值随时间保持固定。我们在这里分析它们变化的配置。我们表明,我们以前的系统的操作可以扩展到处理BQPT和简单的BQSS配置。具有快速演化混合物的BQSS更复杂,因为基本的量子不可克隆定理要求我们分离系统输出的每个可用量子态都不能被复制,从而不能用作(i)后续量子系统的输入,并且(ii)我们分离系统的块不断使用这些状态来更新分离系统的参数值。我们通过引入一个完全不同的BQSS系统来避免这个问题,该系统基于主从结构,并执行并行适应和源状态恢复。因此,所提出的方法是基于自旋电子学来实现所考虑的量子态,并且基于所提出的主从结构中的原始控制回路,由于要处理的信号的量子性质,这需要特定的测量程序。因此,本文弥合了高级信息处理功能(特别是自学习算法)与实现此类计算所需的原子级别定义的物理设备之间的差距。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Blind quantum source separation and process tomography systems for time-varying coupling
Classical, i.e. non-quantum, blind source separation (BSS) methods estimate unknown source signals by using only mixed signals obtained by transferring these source signals through a mixing transform, which typically has unknown parameter values. We developed quantum versions of BSS (called BQSS) and we extended them to the blind estimation of the unknown mixing/coupling parameters, thus achieving blind quantum process tomography (BQPT). In these investigations, the mixing parameter values remained fixed over time. We here analyze configurations where they vary. We show that the operation of our previous system may then be extended to handle BQPT and simple BQSS configurations. BQSS with rapidly evolving mixtures is more complex, because the fundamental quantum no-cloning theorem entails that each quantum state available at the output of our separating system cannot be copied so as to be used as the inputs of both (i) the subsequent quantum system which exploits it and (ii) the block of our separating system which continuously uses these states to update the separating system parameter values. We avoid this issue by introducing a quite different BQSS system, which is based on a master-slave structure and performs parallel adaptation and source state restoration. The proposed approach is thus based on spin electronics for implementing the considered quantum states, and on an original control loop in the proposed master-slave structure, which requires a specific measurement procedure, due to the quantum nature of the signals to be processed. This paper therefore bridges the gap between advanced information processing functions (especially self-learning algorithms) and the physical devices, defined at the atomic level, required for implementing such computations.
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