对于费米 - 哈巴德模型,从优化 ancilla 波函数中得出的极子相关性
Tobias Müller1,2, Ronny Thomale1,3, Subir Sachdev4
1Lehrstuhl für Theoretische Physik I, Institut für Theoretische Physik und Astrophysik and Würzburg-Dresden Cluster of Excellence ct.qmat, Julius-Maximilians-Universität Würzburg, Würzburg 97074, Germany.
概括
这项研究使用变量波函数来模拟Fermi-Hubbard模型中的极子相关性. 这些发现与量子模拟器数据有很好的一致性,捕捉了电子行为的关键交叉.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 量子模拟的量子模拟
- 强烈相关的系统 强烈相关的系统
背景情况:
- 在强烈相关的电子系统中,伪间隙金属相呈现出复杂的电子行为.
- 了解极子相关性对于描述材料中的新兴现象至关重要.
研究的目的:
- 模拟2D费米 - 哈巴德模型中虚空金属相中的极子相关性.
- 将理论预测与超冷原子量子模拟器的实验数据进行比较.
主要方法:
- 采用一个家族的安西拉量子位变化波函数.
- 分析2D费米 - 哈巴德模型在一系列洞中兴奋剂度的范围.
- 将理论结果与量子模拟数据进行比较.
主要成果:
- 在理论建模和量子模拟器数据之间证明了定性和定量一致.
- 成功描述了从半填充到80%洞的极子相关性.
- 捕获了从极子体制到费米液体的观察到的交叉,约有40%的兴奋剂.
结论:
- 安西拉量子位变化波函数提供了对极子相关性的有效描述.
- 这项研究验证了量子模拟器用于研究复杂的凝聚物质模型的使用.
- 这些发现提供了对被杂的Mott绝缘体中电子相位过渡的见解.
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