Abstract

We present a theory of the high-spin generalization of topological insulators and their doped superconducting states. The higher-spin topological insulators involve a pair of $J=3/2$ bands with opposite parity, and are characterized by their band inversion. The low-energy effective theory reveals that the topological insulators host four different phases characterized by mirror Chern numbers, at which boundaries two different patterns of bulk Dirac points appear. For the carrier-doped case, it is shown that the system may host unique unconventional superconductivity because of its high-spin nature and additional orbital degrees of freedom intrinsic to topological insulators. The superconducting critical temperature is evaluated by using density-density pairing interactions, and odd-parity Cooper pairs are shown to be naturally realized in the presence of interorbital pairing interaction. It is observed that even the simplest spin 0 odd-parity pairing state exhibits a novel class of topological superconductivity---high winding topological superconductivity. We also discuss the experimental signals of high winding topological superconductivity in the case of the antiperovskite superconductor Sr$_{3-x}$SnO.

Highlights

  • The search for topological materials is a recent trend in condensed matter physics [1,2,3,4,5,6,7,8]

  • We reveal that the simplest J 1⁄4 0 odd-parity pairing state shows a new class of topological superconductivity, i.e., high winding topological superconductivity

  • We have investigated topological superconductivity in doped topological insulators (TIs) of J 1⁄4 3=2 electrons

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Summary

INTRODUCTION

The search for topological materials is a recent trend in condensed matter physics [1,2,3,4,5,6,7,8]. It has been recognized that multiorbital systems may solve this difficulty, as they allow another mechanism of topological superconductivity [8]: Using interorbital pairing interaction and spin-orbit coupling, a multiorbital system may host odd-parity Cooper pairs even without a strong correlation [18], which indicates topological superconductivity [17,18,19] In this new direction, various types of topological superconductivity in doped topological materials have been discussed recently [18,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37].

Effective Hamiltonian
Octahedral Dirac points
Cubic Dirac points
Oh classification of the gap function
Critical temperatures
TOPOLOGICAL SUPERCONDUCTIVITY IN THE A1u STATE
Mirror Chern numbers
Topological phase diagram
DISCUSSION
Systems without band inversion
Other pairing states
CONCLUSIONS
Nambu space and symmetry
Band representation
Linearized gap equation
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