Experimental and materials considerations for the topological superconducting state in electron and hole doped semiconductors: searching for non-Abelian Majorana modes in 1D nanowires and 2D heterostructures
Jay D. Sau, Sumanta Tewari, S. Das Sarma

TL;DR
This paper investigates how disorder affects the stability of topological superconducting states in doped semiconductors with strong spin-orbit coupling, proposing conditions for realizing Majorana modes in nanowires and heterostructures.
Contribution
It derives an expression for disorder suppression of the superconducting gap and identifies parameter regimes for stable topological states in electron- and hole-doped semiconductors.
Findings
Disorder effects can be minimized by increasing the spin-orbit energy to Zeeman splitting ratio.
Stable topological superconducting states are achievable with realistic parameters.
Suitable semiconductor materials are identified as promising candidates for Majorana mode experiments.
Abstract
In proximity to an s-wave superconductor, a one- or two-dimensional, electron- or hole-doped semiconductor with a sizable spin-orbit coupling and a Zeeman splitting can support a topological superconducting (TS) state. The semiconductor TS state has Majorana fermions as localized zero-energy excitations at order parameter defects such as vortices and sample edges. Here we examine the effects of quenched disorder from the semiconductor surface on the stability of the TS state in both electron- and hole-doped semiconductors. By considering the interplay of broken time reversal symmetry (due to Zeeman splitting) and disorder we derive an expression for the disorder suppression of the superconducting quasiparticle gap in the TS state. We conclude that the effects of disorder can be minimized by increasing the ratio of the spin-orbit energy with the Zeeman splitting. By giving explicit…
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