Topological Superconductivity in Ferromagnetic Metal Chains

Jian Li, Hua Chen, Ilya K. Drozdov, A. Yazdani, B. Andrei Bernevig, A. H. MacDonald

Published 2014-10-13Version 1

Recent experiments have provided evidence that a possible platform for one-dimensional (1D) topological superconductivity, transition metal atom chains formed on a superconducting substrate, can be realized experimentally. We address the properties of this type of system by using a Slater-Koster tight-binding model to account for important features of transition metal electronic structure. We predict that topological superconductivity is nearly universal when ferromagnetic transition metal chains form straight lines on superconducting substrates and that it is possible for more complex chain structures. The proximity induced gap is $\sim \Delta E_{so} / J$ where $\Delta$ is the s-wave pair-potential on the chain, $E_{so}$ is the spin-orbit splitting energy induced in the normal chain state bands by hybridization with the superconducting substrate, and $J$ is the exchange-splitting of the ferromagnetic chain $d$-bands. Because of the topological character of the 1D superconducting state, Majorana end modes appear within the gaps of finite length chains. Pb is a particularly favorable substrate material for ferromagnetic chain topological superconductivity because it provides both strong s-wave pairing and strong Rashba spin-orbit coupling, but there seems to be considerable freedom to optimize the 1D topological superconductivity by varying the atomic composition and structure of the chain. We note that in the absence of disorder a new chain magnetic symmetry, one that is also present in the crystalline topological insulators, can stabilize multiple Majorana modes at the end of a single chain.