在临界点附近的通道期间的非adiabatic过渡
Nikolai A Sinitsyn1, Vijay Ganesh Sadhasivam1,2, Fumika Suzuki1,3
1Theoretical Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
The Journal of chemical physics
|February 16, 2024
概括
这项研究研究了临界点附近的量子系统,揭示了即使没有交叉,缓慢的过渡也会产生非adiabatic刺激. 这项研究得出了激发概率的功率定律前因子,为量子动力学提供了新的见解.
科学领域:
- 量子物理学的量子物理学
- 多体系统是多体系统.
- 非adiabatic动态的动力学
背景情况:
- 量子系统中的临界点通常会导致许多非相应激发.
- 探索那些缓慢地*接近*但没有穿过关键点的系统是不太了解的.
研究的目的:
- 分析在临界点附近,但不相交的多体量子系统中的激发生成.
- 在这种缓慢的,接近临界的过渡中推导激发概率的前因子.
主要方法:
- 适应Dykhne公式用于接近临界点的过渡.
- 非线性兰道-泽纳模型的前因子的导出.
- 介绍一个完全可解决的模型,用于在斯塔克阶梯中的关键点附近的过渡.
主要成果:
- 激发概率的主要指数遵循标准的迪克恩公式参数.
- 指数前因子表现出对过渡率的权力定律依赖.
- 一个完全可解决的斯塔克梯模型显示了质量上类似的激发缩放.
结论:
- 在临界点附近的缓慢过渡,没有交叉,仍然会产生显著的非adiabatic激发.
- 导出的权力规律前因子对于理解这些制度中的激发动态至关重要.
- 这些发现为量子系统在临界现象附近的行为提供了更细致的图片.
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