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两能带系统中激子凝聚的从属转子方法。

Slave rotor approach to exciton condensation in a two-band system.

作者信息

Pradhan Subhasree, Taraphder A

机构信息

Department of Physics, Indian Institute of Technology Kharagpur, Kharagpur-721 302, West Bengal, India. Department of Physics, Jhargram Raj College, Jhragram 721507, West Bengal, India. Department of Physics, Ohio State University, Columbus, OH 43210, United States of America.

出版信息

J Phys Condens Matter. 2019 Jan 9;31(1):015601. doi: 10.1088/1361-648X/aaee06. Epub 2018 Nov 30.

Abstract

We have studied exciton formation and condensation in an extended Falicov-Kimball model, going beyond the weak coupling approach, employing a semi-analytical technique: the slave-rotor mean-field theory (SRMF). In this essentially strong coupling theory, charge and spin (or orbital/pseudospin) degrees are treated as independent degrees of freedom, coupled by a local constraint. Using a two-site-extension of SRMF, we capture the effective many body scale beyond conventional mean-field theory. While the formation of excitons is favoured by the interband hybridization [Formula: see text], it is strongly influenced by the on-site Coulomb interaction [Formula: see text]. Beyond a critical hybridization, there is condensation of excitons, leading to a transition from a metal to an excitonic insulator phase. Moreover, the behaviour of excitonic averages differs from the usual Hartree-Fock mean-field theory. Low-[Formula: see text] results show that excitonic order parameter (Δ) is continuous across the transition both for single as well as two-site approximation, changing to weakly first order one at intermediate [Formula: see text] for the later. The large-[Formula: see text] limit shows a continuous transition for two-site analysis but remains first order in the single-site approximation. The slave rotor theory gives a mixed state of excitons and metal in both the analyses. We have also checked the effect of intersite correlation and localized band hopping on the exciton condensation.

摘要

我们在扩展的法利科夫 - 金博尔模型中研究了激子的形成与凝聚,超越了弱耦合方法,采用了一种半解析技术:从属转子平均场理论(SRMF)。在这个本质上的强耦合理论中,电荷和自旋(或轨道/赝自旋)自由度被视为独立的自由度,并通过一个局部约束相互耦合。通过SRMF的双格点扩展,我们捕捉到了超越传统平均场理论的有效多体尺度。虽然带间杂化[公式:见原文]有利于激子的形成,但它受到在位库仑相互作用[公式:见原文]的强烈影响。超过临界杂化时,会出现激子凝聚,导致从金属相转变为激子绝缘相。此外,激子平均值的行为不同于通常的哈特里 -福克平均场理论。低[公式:见原文]结果表明,对于单格点和双格点近似,激子序参量(Δ)在转变过程中都是连续的,而对于后者,在中间[公式:见原文]时变为弱一级相变。大[公式:见原文]极限表明,双格点分析呈现连续相变,而单格点近似中仍为一级相变。在这两种分析中,从属转子理论都给出了激子和金属的混合态。我们还研究了格点间关联和局域能带跳跃对激子凝聚的影响。

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