Abstract

We propose a general scheme to construct a Hamiltonian $H_{\text{root}}$ describing a square root of an original Hamiltonian $H_{\text{original}}$ based on the graph theory. The square-root Hamiltonian is defined on the subdivided graph of the original graph of $H_{\text{original}}$, where the subdivided graph is obtained by putting one vertex on each link in the original graph. When $H_{\text{original}}$ describes a topological system, there emerge in-gap edge states at non-zero energy in the spectrum of $H_{\text{root}}$, which are the inherence of the topological edge states at zero energy in $H_{\text{original}}$. In this case, $H_{\text{root}}$ describes a square-root topological insulator or superconductor. Typical examples are square roots of the Su-Schrieffer-Heeger (SSH) model, the Kitaev topological superconductor model and the Haldane model. Our scheme is also applicable to non-Hermitian topological systems, where we study an example of a nonreciprocal non-Hermitian SSH model.

Highlights

  • Topological insulators and superconductors are among the most studied fields in condensed matter physics in this decade [1,2]

  • We have presented a systematic method to construct square-root topological insulators and superconductors based on subdivided graphs

  • We recall that subdivided graphs naturally arise in electric circuits when we rewrite the Kirchhoff law in the form of the Schrödinger equation [17,18]

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Summary

INTRODUCTION

Topological insulators and superconductors are among the most studied fields in condensed matter physics in this decade [1,2] They are characterized by the emergence of topological edge states the bulk is gapped. The higher order topological insulator looks trivial since it has no zero-energy edge states. Its notion has been generalized to square-root higher order topological insulators [16] They are characterized by the emergence of in-gap edge states clearly isolated from the bulk band. We find (Hroot )2 = Hpar ⊕ Hres, where Hpar is identical to the original Hamiltonian Horiginal up to an additive constant interpreted as a self-energy. Because the eigenvalues are shown to be identical between Hpar and Hres except for zero-energy states in Hres, Hroot is interpreted as the square-root Hamiltonian of Horiginal. Our results are applicable to non-Hermitian systems, where we demonstrate an example of nonreciprocal non-Hermitian SSH model

SQUARE-ROOT HAMILTONIAN
Square-root SSH model
Square-root Haldane model
Square-root non-Hermitian SSH model
DISCUSSION

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