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]
Summary
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
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