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arXiv 0802.1997quant-phcond-mat.stat-mech
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一维量子游动的大Qudit极限

Large Qudit Limit of One-dimensional Quantum Walks

Mitsunori Sato, Naoki Kobayashi, Makoto Katori, Norio Konno

摘要:

我们研究了Miyazaki { \it et al.}提出的一系列用半整数$j=1/2, 1, 3/2, ...$标记的一维离散时间量子行走模型,其中每一个沃克波函数具有$2j+1$分量,并且在每一个时间步长处的跳跃范围是$2j$。在长时间极限下,赝速度分布的密度函数一般由适当标度的Konno密度函数的叠加给出。由于Konno密度函数有一个有限的开支集,并且在支集的边界处发散,当$2j+1$为偶数时,$(2j+1)$分量模型中赝速度的极限分布可以有$2j+1$峰.然而,当$j$变得很大时,我们发现这些尖峰消失了,并且在极限分布的原点周围出现了一个普遍的单调凸结构。我们讨论了一个可能的路线,从量子行走到经典扩散与$j \to \infty$限制。

英文摘要:

We study a series of one-dimensional discrete-time quantum-walk models labeled by half integers $j=1/2, 1, 3/2, ...$, introduced by Miyazaki {\it et al.}, each of which the walker's wave function has $2j+1$ components and hopping range at each time step is $2j$. In long-time limit the density functions of pseudovelocity-distributions are generally given by superposition of appropriately scaled Konno's density function. Since Konno's density function has a finite open support and it diverges at the boundaries of support, limit distribution of pseudovelocities in the $(2j+1)$-component model can have $2j+1$ pikes, when $2j+1$ is even. When $j$ becomes very large, however, we found that these pikes vanish and a universal and monotone convex structure appears around the origin in limit distributions. We discuss a possible route from quantum walks to classical diffusion associated with the $j \to \infty$ limit.

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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