Abstract

In this paper, the authors find a family of in-gap chiral edge states in non-inverted spin-1 Dirac quantum dots, which represent a topologically trivial confinement configuration. This finding uncovers that topologically protected states can arise in condensed matter systems even without topological restriction, opening a wider avenue for applications of topological quantum states.

Highlights

  • A fundamental principle in the study of topological phases of matters is the bulk-edge correspondence [1,2], which states that robust interfacial modes immune to impurities or geometric perturbations can arise on the boundary between domains with distinct bulk topological invariants

  • The principle was originally discovered in electronic systems, but in recent years topological states and the bulk-edge correspondence have been extended to a broad range of fields in physics, from cold atoms [3], optics and photonics [4], to classical fluid and solid mechanics [5]

  • The results indicate that the unconventional chiral edge states without engaging any topological band inversion have a comparable level of robustness as the conventional topological states with band inversion

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Summary

INTRODUCTION

A fundamental principle in the study of topological phases of matters is the bulk-edge correspondence [1,2], which states that robust interfacial modes immune to impurities or geometric perturbations can arise on the boundary between domains with distinct bulk topological invariants. Quantum materials hosting a flat band, such as the magic-angle twisted bilayer graphene, have become a forefront area of research These materials can generate remarkable physical phenomena such as unconventional superconductivity [39,40], orbital ferromagnetism [41,42], and Chern insulating behavior with topological edge states. Our setting is the generic mesoscopic structure of quantum dot for massive spin-1 Dirac particles arising in materials with an energy gap. The corresponding topological invariant describes a quantum dot system with or without an inverted band alignment The former case is conventional and has been known to host topologically protected chiral edge modes in the gap [45,46]. In sharp contrast to the conventional wisdom, we find that such states can arise for spin-1 Dirac particles and are remarkably robust against geometric perturbations

RESULTS
Unconventional chiral edge states without band inversion
Robustness
Spin-1 Fock-Darwin and Landau-level states
REGULARIZATIOIN ASSOCIATED WITH BULK TOPOLOGY AND BULK-EDGE CORRESPONDENCE
Anamalous chiral edge modes in noninverted lattice spin-1 quantum dots
CONCLUSION AND DISCUSSION
Basics
Eigensolutions of dot confinement without magnetic field
Landau levels and confinement in the presence of a magnetic field
Implementation
Method validation
Full Text
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