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arXiv quant-ph/0408140quant-ph
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直线上连续时间量子行走的极限定理

Limit Theorem for Continuous-Time Quantum Walk on the Line

Norio Konno

摘要:

本文作者证明了,对于离散时间量子游走X^{(d)} t,其演化用Hadamard变换描述,弱极限定理成立:X^{(d)} t /\to dx / π(1-x^2)\sqrt{1 - 2 x^2} as \to \infty .本文证明了对于{ \it连续时间}量子行走X^{(c)}_t满足类似的弱极限定理:X^{(c)}_t /tPDMATHABMM dx / π \sqrt{1 - x^2} as \to \infty .量子游动的这些结果与对称离散和连续时间经典随机游动的中心极限定理形成了鲜明的对比:Y_{t} / \sqrt{t} \to e^{-x^2/2} dx / \sqrt{2 π} as t PDMATHAMM \infty。工作还涉及离散和连续时间量子行走之间的关系的问题。这一主题,在以前的文献中的一个长期的辩论的主题,在矩阵表示的形式主义和极限分布进行了详尽的比较,在这两种情况下。

英文摘要:

Concerning a discrete-time quantum walk X^{(d)}_t with a symmetric distribution on the line, whose evolution is described by the Hadamard transformation, it was proved by the author that the following weak limit theorem holds: X^{(d)}_t /t \to dx / π(1-x^2) \sqrt{1 - 2 x^2} as t \to \infty. The present paper shows that a similar type of weak limit theorems is satisfied for a {\it continuous-time} quantum walk X^{(c)}_t on the line as follows: X^{(c)}_t /t \to dx / π\sqrt{1 - x^2} as t \to \infty. These results for quantum walks form a striking contrast to the central limit theorem for symmetric discrete- and continuous-time classical random walks: Y_{t}/ \sqrt{t} \to e^{-x^2/2} dx / \sqrt{2 π} as t \to \infty. The work deals also with issue of the relationship between discrete and continuous-time quantum walks. This topic, subject of a long debate in the previous literature, is treated within the formalism of matrix representation and the limit distributions are exhaustively compared in the two cases.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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