Abstract

We investigate the roles of symmetry and bulk-boundary correspondence in characterizing topological edge states in generalized Jackiw–Rebbi (JR) models. We show that time-reversal (T), charge-conjugation (C), parity (P), and discrete internal field rotation (Z_n) symmetries protect and characterize the various types of edge states such as chiral and nonchiral solitons via bulk-boundary correspondence in the presence of the multiple vacua. As two representative models, we consider the JR model composed of a single fermion field having a complex mass and the generalized JR model with two massless but interacting fermion fields. The JR model shows nonchiral solitons with the Z_2 rotation symmetry, whereas it shows chiral solitons with the broken Z_2 rotation symmetry. In the generalized JR model, only nonchiral solitons can emerge with only Z_2 rotation symmetry, whereas both chiral and nonchiral solitons can exist with enhanced Z_4 rotation symmetry. Moreover, we find that the nonchiral solitons have C, P symmetries while the chiral solitons do not, which can be explained by the symmetry-invariant lines connecting degenerate vacua. Finally, we find the symmetry correspondence between multiply-degenerate global vacua and solitons such that T, C, P symmetries of a soliton inherit from global minima that are connected by the soliton, which provides a novel tool for the characterization of topological solitons.

Highlights

  • We investigate the roles of symmetry and bulk-boundary correspondence in characterizing topological edge states in generalized Jackiw–Rebbi (JR) models

  • We find that the enhanced Z4 rotation symmetry supports the emergence of chiral and nonchiral solitons

  • In right chiral (RC) and left chiral (LC) soliton systems, C and P symmetries are broken because the bose fields deviate from the symmetry-invariant line, which naturally endows the chirality to solitons

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Summary

Introduction

We investigate the roles of symmetry and bulk-boundary correspondence in characterizing topological edge states in generalized Jackiw–Rebbi (JR) models. We show that the cooperation of time-reversal, charge-conjugation, parity, and discrete field rotation ( Zn ) symmetries protects and identifies the various types of soliton states via bulk-boundary correspondence. The JR model shows charge-conjugate and parity-invariant solitons (equivalently, nonchiral solitons) in the presence of Z2 field rotation symmetry, otherwise it shows chiral solitons with broken C and P symmetries.

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