Abstract

Modern theory of electric polarization is formulated by the Berry phase, which, when quantized, leads to topological phases of matter. Such a formulation has recently been extended to higher electric multipole moments, through the discovery of the so-called quadupole topological insulator. It has been established by a classical electromagnetic theory that in a two-dimensional material the quantized properties for the quadupole topological insulator should satisfy a basic relation. Here we discover a new type of quadrupole topological insulator (dubbed type-II) that violates this relation due to the breakdown of the correspondence that a Wannier band and an edge energy spectrum close their gaps simultaneously. We find that, similar to the previously discovered (referred to as type-I) quadrupole topological insulator, the type-II hosts topologically protected corner states carrying fractional corner charges. However, the edge polarizations only occur at a pair of boundaries in the type-II insulating phase, leading to the violation of the classical constraint. We demonstrate that such new topological phenomena can appear from quench dynamics in non-equilibrium systems, which can be experimentally observed in ultracold atomic gases. We also propose an experimental scheme with electric circuits to realize such a new topological phase of matter. The existence of the new topological insulating phase means that new multipole topological insulators with distinct properties can exist in broader contexts beyond classical constraints.

Highlights

  • The formulation of electric polarization based on the Berry phase has been extended to higher electric multipole moments, such as quadrupole moments and octupole moments [1,2]

  • The edge polarizations only occur at a pair of boundaries in the type-II insulating phase, leading to the violation of the classical constraint. We demonstrate that such new topological phenomena can appear from quench dynamics in non-equilibrium systems, which can be experimentally observed in ultracold atomic gases

  • We propose an experimental scheme with electric circuits to realize such a new topological phase of matter

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Summary

INTRODUCTION

The formulation of electric polarization based on the Berry phase has been extended to higher electric multipole moments, such as quadrupole moments and octupole moments [1,2]. We find another new topological phase with quantized edge polarizations but without zeroenergy corner modes and quadrupole moments This transition arises from the relevant Wannier gap closing characterized by the change of the winding number for a Wilson line. [1] introduces a three-dimensional higher-order topological insulator by breaking the reflection symmetries so that the quadrupole moment, edge polarizations at all boundaries and corner charges all exhibit a winding, which is associated with the presence of chiral hinge modes. We construct several significantly simplified models supporting the type-II QTI We present another topological phase with quantized edge polarizations but without zero-energy corner modes and quadrupole moments.

THE TYPE-II QTI
A TOPOLOGICAL INVARIANT FOR A WILSON LINE
A general analysis
Simplified models for the type-II QTI
HI I I
An alternative approach to show the inequivalence
PUMPING PHENOMENA AND NOVEL
QUENCH DYNAMICS
EXPERIMENTAL REALIZATION
VIII. CONCLUSION
Generic symmetry constraint of a Wilson line
Reflection symmetry constraint and topological invariants
Gauge transformation
Full Text
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