Abstract

Electron–electron interactions can be useful for realizing new nontrivial topological phases of matter. Here, we show by means of a tight-binding model and mean field theory how electron–electron interactions can lead to a topological phase transition. By externally adding or removing electrons from the system a band inversion between two bands with different parity is induced. This leads to a topological nontrivial phase if spin–orbit coupling is present. Besides the toy-model illustrating this mechanism, we also propose SmB6 as a possible playground for experimentally realizing a topological phase transition by external tuning.

Highlights

  • Electron–electron interactions in material systems give rise to rich phase diagrams and offer the possibility to tune between those phases by for example doping [1,2,3]

  • In this system spin–orbit coupling is unnecessary for a topological nontrivial phase and can be replaced by electron–electron interactions

  • We show how a system with spin–orbit interaction and a Hubbard U like electron–electron interaction can lead to a topological phase transition

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Summary

Introduction

Electron–electron interactions in material systems give rise to rich phase diagrams and offer the possibility to tune between those phases by for example doping [1,2,3]. Raghu et al [22], reported a system in which nearest and next-nearest neighbour Coulomb repulsion leads to spontaneous symmetry breaking, resulting in a system similar to Haldane [23] In this system spin–orbit coupling is unnecessary for a topological nontrivial phase and can be replaced by electron–electron interactions. We show how a system with spin–orbit interaction and a Hubbard U like electron–electron interaction can lead to a topological phase transition This simple toy-model shows the basic principle behind a ‘interaction driven phase transition’, which applies to other systems were spin–orbit coupling is still a driving force.

Tuning by electron filling
SmB6 as possible playground
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