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arXiv 1009.2019quant-ph
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随机硬币量子游动的渐近演化

Asymptotic evolution of quantum walks with random coin

Andre Ahlbrecht, Holger Vogts, Albert H. Werner, Reinhard F. Werner

摘要:

研究了格上一般量子游动的渐近位置分布,包括随机硬币的游动,随机硬币是由一般马氏链逐步选择的。在一元(即,非随机)的情况下,我们允许任何幺正算子,它与平移交换,并且仅耦合彼此相距有限距离的站点。例如,行走的单个步骤可以由通常意义上的不同移位和硬币操作的任何有限序列组成,具有任何格维数和硬币维数。我们发现弹道标度,并建立一个直接的方法来计算的渐近分布的位置除以时间,即作为离散时间模拟群速度的分布。在随机情况下,我们让一个马尔可夫链(控制过程)在每一步中从上面描述的意义上的200多个酉游动中挑选一个。在弹道顺序,我们发现一个非随机漂移,这只取决于控制过程的平均值,而不是在初始状态。在扩散尺度中,极限分布是渐近高斯分布,协方差矩阵(扩散矩阵)取决于动量。扩散矩阵不仅依赖于控制过程的平均值,而且依赖于控制过程的转移率。在非随机极限中,即,当所选择的硬币都非常接近或控制过程的转变速率很小时,导致弹道演变的长间隔,扩散矩阵发散。我们的方法是基于空间傅里叶变换,和一阶和二阶微扰理论的特征值1的过渡算子的每个值的动量。

英文摘要:

We study the asymptotic position distribution of general quantum walks on a lattice, including walks with a random coin, which is chosen from step to step by a general Markov chain. In the unitary (i.e., non-random) case, we allow any unitary operator, which commutes with translations, and couples only sites at a finite distance from each other. For example, a single step of the walk could be composed of any finite succession of different shift and coin operations in the usual sense, with any lattice dimension and coin dimension. We find ballistic scaling, and establish a direct method for computing the asymptotic distribution of position divided by time, namely as the distribution of the discrete time analog of the group velocity. In the random case, we let a Markov chain (control process) pick in each step one of finitely many unitary walks, in the sense described above. In ballistic order we find a non-random drift, which depends only on the mean of the control process and not on the initial state. In diffusive scaling the limiting distribution is asymptotically Gaussian, with a covariance matrix (diffusion matrix) depending on momentum. The diffusion matrix depends not only on the mean but also on the transition rates of the control process. In the non-random limit, i.e., when the coins chosen are all very close, or the transition rates of the control process are small, leading to long intervals of ballistic evolution, the diffusion matrix diverges. Our method is based on spatial Fourier transforms, and the first and second order perturbation theory of the eigenvalue 1 of the transition operator for each value of the momentum.

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