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非中心对称晶体中电子相互作用产生的非互易电流:时间反演对称性和耗散的作用。

Nonreciprocal current from electron interactions in noncentrosymmetric crystals: roles of time reversal symmetry and dissipation.

作者信息

Morimoto Takahiro, Nagaosa Naoto

机构信息

Department of Physics, University of California, Berkeley, CA, 94720, USA.

RIKEN Center for Emergent Matter Science (CEMS), Wako, Saitama, 351-0198, Japan.

出版信息

Sci Rep. 2018 Feb 14;8(1):2973. doi: 10.1038/s41598-018-20539-2.

Abstract

In noncentrosymmetric crystals with broken inversion symmetry [Formula: see text], the I-V (I: current, V: voltage) characteristic is generally expected to depend on the direction of I, which is known as nonreciprocal response and, for example, found in p-n junction. However, it is a highly nontrivial issue in translationally invariant systems since the time-reversal symmetry T plays an essential role, where the two states at crystal momenta k and -k are connected in the band structure. Therefore, it has been considered that the external magnetic field (B) or the magnetic order which breaks the T-symmetry is necessary to realize the nonreciprocal I-V characteristics, i.e., magnetochiral anisotropy. Here we theoretically show that the electron correlation in T-broken multi-band systems can induce nonreciprocal I-V characteristics without T-breaking. An analog of Onsager's relation shows that nonreciprocal current response without T -breaking generally requires two effects: dissipation and interactions. By using nonequilibrium Green's functions, we derive general formula of the nonreciprocal response for two-band systems with onsite interaction. The formula is applied to Rice-Mele model, a representative 1D model with inversion breaking, and some candidate materials are discussed. This finding offers a coherent understanding of the origin of nonreciprocal I-V characteristics, and will pave a way to design it.

摘要

在具有反演对称性破缺[公式:见原文]的非中心对称晶体中,通常预期电流 - 电压(I:电流,V:电压)特性取决于电流方向,这被称为非互易响应,例如在 p - n 结中可以发现。然而,在平移不变系统中这是一个非常复杂的问题,因为时间反演对称性 T 起着至关重要的作用,在能带结构中晶体动量 k 和 -k 处的两个状态是相连的。因此,人们认为打破 T 对称性的外部磁场(B)或磁序对于实现非互易电流 - 电压特性(即磁手性各向异性)是必要的。在这里,我们从理论上表明,在打破 T 对称性的多带系统中的电子关联可以在不打破 T 对称性的情况下诱导出非互易电流 - 电压特性。类似于昂萨格关系表明,不打破 T 对称性的非互易电流响应通常需要两种效应:耗散和相互作用。通过使用非平衡格林函数,我们推导了具有在位相互作用的双带系统的非互易响应的一般公式。该公式应用于具有反演对称性破缺的代表性一维模型——赖斯 - 梅勒模型,并讨论了一些候选材料。这一发现为非互易电流 - 电压特性的起源提供了连贯的理解,并将为其设计铺平道路。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e9ff/5813057/35c48e0c745c/41598_2018_20539_Fig1_HTML.jpg

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