相关实验视频
Updated: Jun 28, 2025

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Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
Published on: March 30, 2017
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片绝缘体和格子费米子
Thomas Iadecola1,2, Srimoyee Sen1, Lars Sivertsen1
1Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA.
Physical review letters
|April 13, 2024
概括
定期运行Floquet绝缘体揭示了新的拓阶段. 这些阶段模仿费米子的翻倍,映射到离散时间格子费米子理论与减少空间站点.
科学领域:
- 量子物理学的量子物理学
- 凝聚物质物理学 凝聚物质物理学
- 拓阶段 拓阶段是指拓阶段.
背景情况:
- 方块绝缘器是经过周期性驱动的量子系统,导致独特的拓相.
- 这些相与离散时间格子费米子理论中观察到的费米子倍增现象有共同的特征.
研究的目的:
- 具体证明Floquet绝缘体相与离散时间格子费米子理论之间的联系.
- 将一个特定的Floquet绝缘体模型的光谱特性映射到一个时间独立的哈密尔顿式.
主要方法:
- 在特定的驱动参数下分析非相互作用的 (1+1) D 浮板绝缘体的光谱.
- 将这个光谱映射到一个离散时间格子费米子理论上,具有时间独立的哈密尔顿式.
主要成果:
- 绘制的结果是一个哈密尔顿式,与斯特罗波斯科普的Floquet哈密尔顿式不同.
- 衍生的哈密尔顿式可以表示一个离散时间的苏-施里弗-希格尔模型,其中有一半是原来的空间位点.
- 或者,它可以表现为 (1+1) D威尔逊-迪拉克理论,其中四分之一的原始空间站点.
结论:
- 定期驱动的Floquet绝缘器可以有效实现离散时间格子费米子模型.
- 这为驱动量子系统中的拓相及其与格子场理论的关系提供了新的视角.
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