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arXiv 2011.02778quant-phmath-phmath.MP
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系统子空间时间演化的量子速度极限

Quantum speed limits for time evolution of a system subspace

Sergio Albeverio, Alexander K. Motovilov

摘要:

量子态时间演化速度的基本物理极限之一是著名的曼德尔斯塔姆-塔姆不等式。这个不等式回答了一个孤立的量子系统从初始态到正交态的演化速度有多快的问题。反过来,弗莱明界是Mandelstam-Tamm不等式的扩展,它给出了非正交初始和最终状态之间演化的最佳速度界。在目前的工作中,我们所关心的不是一个单一的状态,但与整个(可能是无限维)子空间的系统状态,受到薛定谔演化。通过使用子空间之间的最大角度的概念,我们得到这样的子空间演化的速度,可以被看作是一个自然的推广弗莱明界的最佳估计。

英文摘要:

One of the fundamental physical limits on the speed of time evolution of a quantum state is known in the form of the celebrated Mandelstam-Tamm inequality. This inequality gives an answer to the question on how fast an isolated quantum system can evolve from its initial state to an orthogonal one. In its turn, the Fleming bound is an extension of the Mandelstam-Tamm inequality that gives an optimal speed bound for the evolution between non-orthogonal initial and final states. In the present work, we are concerned not with a single state but with a whole (possibly infinite-dimensional) subspace of the system states that are subject to the Schroedinger evolution. By using the concept of maximal angle between subspaces we derive an optimal estimate on the speed of such a subspace evolution that may be viewed as a natural generalization of the Fleming bound.

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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