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测量诱导的量子行走。

Measurement-induced quantum walks.

作者信息

Didi A, Barkai E

机构信息

Department of Physics, Institute of Nanotechnology and Advanced Materials, Bar-Ilan University, Ramat-Gan 5290002, Israel.

出版信息

Phys Rev E. 2022 May;105(5-1):054108. doi: 10.1103/PhysRevE.105.054108.

Abstract

We investigate a tight-binding quantum walk on a graph. Repeated stroboscopic measurements of the position of the particle yield a measured "trajectory," and a combination of classical and quantum mechanical properties for the walk are observed. We explore the effects of the measurements on the spreading of the packet on a one-dimensional line, showing that except for the Zeno limit, the system converges to Gaussian statistics similarly to a classical random walk. A large deviation analysis and an Edgeworth expansion yield quantum corrections to this normal behavior. We then explore the first passage time to a target state using a generating function method, yielding properties like the quantization of the mean first return time. In particular, we study the effects of certain sampling rates that cause remarkable changes in the behavior in the system, such as divergence of the mean detection time in finite systems and decomposition of the phase space into mutually exclusive regions, an effect that mimics ergodicity breaking, whose origin here is the destructive interference in quantum mechanics. For a quantum walk on a line, we show that in our system the first detection probability decays classically like (time)^{-3/2}. This is dramatically different compared to local measurements, which yield a decay rate of (time)^{-3}, indicating that the exponents of the first passage time depend on the type of measurements used.

摘要

我们研究了图上的紧束缚量子行走。对粒子位置进行重复的频闪测量会产生一个测量到的“轨迹”,并且观察到该行走的经典和量子力学性质的组合。我们探究了测量对一维直线上波包扩散的影响,结果表明,除了芝诺极限外,该系统与经典随机行走类似地收敛到高斯统计。大偏差分析和埃奇沃思展开给出了对这种正态行为的量子修正。然后,我们使用生成函数方法探究到达目标态的首次通过时间,得到诸如平均首次返回时间的量子化等性质。特别地,我们研究了某些采样率的影响,这些采样率会导致系统行为发生显著变化,例如有限系统中平均检测时间的发散以及相空间分解为相互排斥的区域,这种效应类似于遍历性破缺,其根源在于量子力学中的相消干涉。对于直线上的量子行走,我们表明在我们的系统中首次检测概率按经典方式像(时间)^{-3/2}那样衰减。这与局部测量有显著不同,局部测量产生的衰减率为(时间)^{-3},这表明首次通过时间的指数取决于所使用的测量类型。

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