Abstract

The recent discovery of topological superconductors (TSCs) has sparked enormous interest. The realization of TSC requires a delicate tuning of multiple microscopic parameters, which remains a great challenge. Here, we develop a first-principles approach to quantify realistic conditions of TSC by solving self-consistently Bogoliubov-de Gennes equation based on a Wannier function construction of band structure, in presence of Rashba spin-orbit coupling, Zeeman splitting and electron-phonon coupling. We further demonstrate the power of this method by predicting the Mn-doped GeTe (Ge1-xMnxTe) monolayer—a well-known dilute magnetic semiconductor showing superconductivity under hole doping—to be a Class D TSC with Chern number of −1 and chiral Majorana edge modes. By constructing a first-principles phase diagram in the parameter space of temperature and Mn concentration, we propose the TSC phase can be induced at a lower-limit transition temperature of ~40 mK and the Mn concentration of x~0.015%. Our approach can be generally applied to TSCs with a phonon-mediated pairing, providing useful guidance for future experiments.

Highlights

  • The topological phase of superconductors (SC) has recently received intense research interest as the superconducting quasiparticles residing in the non-trivial gapless/zero-energy boundary states are considered a form of Majorana fermions

  • We demonstrate the usefulness of this method by predicting the Mn-doped GeTe (Ge1-xMnxTe) monolayer to be a topological superconductors (TSCs) by constructing a firstprinciples phase diagram in the parameter space of temperature and Mn concentration

  • The firstprinciples Bogoliubov-de Gennes (BdG) Hamiltonian was constructed via a Wannier function (WF) scheme, through which we found that the GeTe monolayer with the hole concentration of ~7.4 × 1013 cm−2 becomes superconducting below ~120 mK and the Ge1-xMnxTe monolayer is a Class D TSC with Tc~40 mK characterized by a non-zero Chern number and chiral Majorana edge modes

Read more

Summary

INTRODUCTION

The topological phase of superconductors (SC) has recently received intense research interest as the superconducting quasiparticles residing in the non-trivial gapless/zero-energy boundary states are considered a form of Majorana fermions. Intrinsic TSCs exhibit inherently a nontrivial superconducting gap without the need of applying an external field or constructing a heterostructure They may be pwave SCs with natural spin-triplet pairing[18,19], such as Sr2RuO420, Cu/Sr/Nb-doped Bi2Se321 and non-centrosymmetric SCs22, or swave SCs with an effective spin-triplet pairing resulting from helical spin-polarized states, such as the two-dimensional (2D) topological electronic states[23,24], and 1D25,26 and 2D Rashba electronic states[27,28,29] which belong to the so-called Class D TSC without time-reversal symmetry (TRS).

Zhang et al 2
RESULTS AND DISCUSSION
F Z D2F Z
METHODS
NF ωqv
CODE AVAILABILITY
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call