哈伯德模型中的电子配对是现场排斥力波动的结果

I. N. Karnaukhov
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引用次数: 1

摘要

我们将定量分析的重点放在半填充时Hubbard模型中绝缘体状态的稳定性上。考虑到现场排斥的宏观波动,我们考虑了实现以电子配对为特征的稳态的可能性。现场斥力的波动导致空穴以激发态的形式形成。电子液体在具有裸场排斥U的状态下有两种弛豫的可能性:平凡的初始状态,和非平凡的电子极化空穴形成电子-空穴对的状态。稳态是由给定U的最小能量及其波动δU决定的。计算了具有电子配对的态是稳定的U和δU值。所提出的配对机制在某种程度上类似于光学诱导的哈伯德链中长程配对相关性的形成[]。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Electron pairing in the Hubbard model as a result of on-site repulsion fluctuations
We focus our quantitative analysis on the stability of insulator state in the Hubbard model at half-filling. Taking into account macroscopic fluctuation of the on-site repulsion, we consider the possibility of realizing a steady state which is characterized by electron pairing. Fluctuation of the on-site repulsion leads to the formation of holes in the form of excited states. The electron liquid has two possibilities of relaxation in the state with bare on-site repulsion U: trivial, to the initial state, and nontrivial to state in which electrons polarize holes forming electron-hole pairs. A steady state is determined by minimum energy for given U and its fluctuation δU . The values U and δU , for which the states with electron pairing are stable, are calculated. The proposed pairing mechanism is to some extent similar to the formation of a long-range pairing correlation in an optically induced Hubbard chain [].
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