强烈的多体定位在相互作用的无限维系统中
Hristiana Atanasova1, André Erpenbeck2, Emanuel Gull2
1School of Chemistry, Tel Aviv University, Tel Aviv 6997801, Israel.
Physical review letters
|May 3, 2024
概括
费米-哈伯德模型中的粒子运输在弱电场中显示正常扩散. 随着电场的增加,传输变得分扩散,然后超扩散,在局部化发生之前,抑制电流.
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.
- 统计力学 统计力学
背景情况:
- 之前对1D类型的研究表明,斯塔克的多体局部化阻碍了扩散.
- 了解驱动量子系统中的粒子传输对于它们的技术应用至关重要.
研究的目的:
- 在Fermi-Hubbard模型中,在电场下的Bethe格子上研究散装粒子运输.
- 描述从扩散到局部化运输制度的过渡.
- 分析电场强度和相互作用强度对运输动态的影响.
主要方法:
- 使用了数字精确和近似技术的组合.
- 研究的系统最初是在旋转密度波状态下准备的.
- 分析了波的动量组成部分随着时间的推移的衰减.
主要成果:
- 对于弱电场,观察到正常的扩散,动量呈指数式衰减.
- 发现了动态指数与电场强度的非单调依赖.
- 随着电场的增加,运输从亚扩散转变为超扩散,最终导致局部化.
结论:
- 在Bethe格子上的费米-哈伯德模型在电场下表现出复杂的运输行为.
- 电场和相互作用强度之间的相互作用决定了传输模式.
- 强烈的多体定位可以抑制这些驱动量子系统中的电流.
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