在多频段布洛赫哈密尔顿的周期动态量子相位过渡及其起源
Kaiyuan Cao1, Hao Guo2, Guangwen Yang1,3
1Research Center for Intelligent Supercomputing, Zhejiang Lab, Hangzhou 311100, People's Republic of China.
概括
研究人员在1D基塔耶夫模型中探索了动态量子相位过渡 (DQPT). 多频带效应导致非周期性关键时间,与更简单的模型不同,DQPTs需要带间隙崩.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 量子力学就是量子力学.
- 材料科学 材料科学 材料科学
背景情况:
- 动态量子相位转换 (DQPT) 是一种非平衡现象.
- 一维周期性基塔耶夫模型是研究拓相的一个关键系统.
- 多频段的哈密尔顿模型引入了在更简单的双频段模型中不存在的复杂性.
研究的目的:
- 在布洛赫频段灭下,研究多频段1D基塔耶夫模型中的DQPT.
- 分析多频段效应对DQPT关键时间和发生的影响.
- 在这个背景下探索拓顺序参数的性质.
主要方法:
- 动态自由能量的分析.
- 潘查拉特南几何相 (PGP) 的计算.
- 在多波段哈密尔顿式中研究来自布洛赫状态的火.
主要成果:
- 由于多频带效应,DQPT的关键时间表现出非周期间隔.
- DQPTs仅发生在灭崩带间隙时.
- 基于PGP上数的动态拓顺序参数是不定量化的,但显示了不连续性.
- 在零度以外的温度下,混合状态的DQPT不存在.
结论:
- 与两带模型相比,多带效应显著改变了DQPT动态.
- 一个几何解释解释了关键时间的非均间距.
- 在这个系统中,带间隙崩是DQPT的必要条件.
- 该研究提供了对非平衡拓现象及其表征的见解.
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