在局部超标系统中,从局部到统一的编码的动态过渡
Mathias Steinhuber1, Peter Schlagheck2, Juan Diego Urbina1
1Institut für Theoretische Physik, Universität Regensburg, 93040 Regensburg, Germany.
Physical review. E
|September 19, 2023
概括
量子系统根据初始状态表现出不同的混速率. 这项研究揭示了波包杂乱中的动态过渡,将不稳定的分离力学动态与混乱区分开来.
科学领域:
- 量子动力学就是量子动力学.
- 统计力学就是统计力学.
- 这是量子混沌.
背景情况:
- 量子相关性的快速杂乱,通过时间外顺序相关器 (OTOC) 测量,是不稳定动态的量子特征.
- 之前的研究表明,可集成系统的编码速率不同,取决于初始状态的本地化.
研究的目的:
- 研究量子系统中波包杂乱的动态过渡.
- 提供了一个物理图像,用于观察到的杂乱率的交叉.
- 使用OTOCs区分不稳定的分离力学与混乱的动态.
主要方法:
- 分析性的半古典方法.
- 在Bose-Hubbard二进制模型上的数值模拟.
- 对量子利亚普诺夫指数 (λq) 和稳定指数 (λs) 的分析.
主要成果:
- 一个波包最初定位在一个不稳定的固定点周围,显示了混速率的动态过渡.
- 量子Lyapunov指数在2λs和λs之间进行过渡.
- 这种交叉被认为是不稳定的分离力学动态的标志.
结论:
- 在OTOC增长中观察到的动态过渡作为一个独特的签名.
- 这一发现允许在可整合系统中区分不稳定的分离动力学与一般的混乱动力学.
- 这项研究为表征量子系统动态提供了一个新的可观测值.
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