Abstract

Topological superconductors (TSCs) are correlated quantum states with simultaneous off-diagonal long-range order and nontrivial topological invariants. They produce gapless or zero energy boundary excitations, including Majorana zero modes and chiral Majorana edge states with topologically protected phase coherence essential for fault-tolerant quantum computing. Candidate TSCs are very rare in nature. Here, we propose a novel route toward emergent quasi-one-dimensional (1D) TSCs in naturally embedded quantum structures such as atomic line defects in unconventional spin-singlet $s$-wave and $d$-wave superconductors. We show that inversion symmetry breaking and charge transfer due to the missing atoms lead to the occupation of incipient impurity bands and mixed parity spin singlet and triplet Cooper pairing of neighboring electrons traversing the line defect. Nontrivial topological invariants arise and occupy a large part of the parameter space, including the time reversal symmetry breaking Zeeman coupling due to applied magnetic field or defect-induced magnetism, creating TSCs in different topological classes with robust Majorana zero modes at both ends of the line defect. Beyond providing a novel mechanism for the recent discovery of zero-energy bound states at both ends of an atomic line defect in monolayer Fe(Te,Se) superconductors, the findings pave the way for new material realizations of the simplest and most robust 1D TSCs using embedded quantum structures in unconventional superconductors with large pairing energy gaps and high transition temperatures.

Highlights

  • Superfluid and superconductors are fundamental quantum states exhibiting off-diagonal long-range order [1,2]

  • We presented a new route for materializing quasi-1D topological superconductors using naturally embedded quantum structures, such as the Rashba atomic line defects, in spin-singlet unconventional superconductors

  • This advantage avoids relying on proximity-effect-induced superconductivity that is difficult to achieve and hard to control in unconventional superconductors and, at the same time, brings out the crystalline symmetry for the emergent Topological superconductors (TSCs) to be reckoned with

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Summary

INTRODUCTION

Superfluid and superconductors are fundamental quantum states exhibiting off-diagonal long-range order [1,2]. We report here that quasi-1D TSCs of mixed parity in multiple topological classes can emerge in naturally embedded quantum structures, such as an atomic line defect, in unconventional spin-singlet superconductors with high transition temperature (Tc) and large pairing energy gaps. Occupations of more impurity bands may occur more generally [36] Because of these unique properties of the embedded quantum structure, the coupling of the RALD to the bulk unconventional superconductor can be described microscopically by the coherent processes of hopping, pairing, and spinorbit coupling, leading to the induced quasi-1D mixedparity pairing states on the RALD in a systematic and controllable manner. We present the 2D model describing the impurity bands along the RALD and its couplings to the bulk superconductor in Sec. III and discuss the results obtained directly from the 2D unconventional superconductors with the embedded quantum structure.

EFFECTIVE 1D THEORY FOR EMBEDDED RALD
QUASI-1D TSC FROM EMBEDDED RALD IN 2D UNCONVENTIONAL SUPERCONDUCTORS
TSC from RALD embedded in s-wave superconductors
Even-parity-dominated quasi-1D TSC
Odd-parity-dominated quasi-1D TSC
General quasi-1D TSC of mixed parity
TSC from RALD embedded in d-wave superconductors
RALD embedded along antinodal directions
RALD embedded along nodal directions
ZEEMAN EFFECT AND TIME-REVERSAL SYMMETRY-BREAKING TSC
Mirror symmetric RALD
Mirror-symmetry-breaking RALD
Nodal RALD embedded in d-wave superconductors
SUMMARY AND OUTLOOK
Time-reversal-symmetric case
Time-reversal symmetry-breaking case
Chiral symmetric case
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