Topological superconductivity of spin-3/2 carriers in a three-dimensional doped Luttinger semimetal
arXiv:1708.07825 · doi:10.1103/PhysRevB.99.054505
Abstract
We investigate topological Cooper pairing, including gapless Weyl and fully gapped class DIII superconductivity, in a three-dimensional doped Luttinger semimetal. The latter describes effective spin-3/2 carriers near a quadratic band touching and captures the normal-state properties of the 227 pyrochlore iridates and half-Heusler alloys. Electron-electron interactions may favor non--wave pairing in such systems, including even-parity -wave pairing. We argue that the lowest energy -wave pairings are always of complex (e.g., ) type, with nodal Weyl quasiparticles. This implies scaling of the density of states (DoS) at low energies in the clean limit, or over a wide critical region in the presence of disorder. The latter is consistent with the -dependence of the penetration depth in the half-Heusler compound YPtBi. We enumerate routes for experimental verification, including specific heat, thermal conductivity, NMR relaxation time, and topological Fermi arcs. Nucleation of any -wave pairing also causes a small lattice distortion and induces an -wave component; this gives a route to strain-engineer exotic pairings. We also consider odd-parity, fully gapped -wave superconductivity. For hole doping, a gapless Majorana fluid with cubic dispersion appears at the surface. We invent a generalized surface model with -fold dispersion to simulate a bulk with winding number . Using exact diagonalization, we show that disorder drives the surface into a critically delocalized phase, with universal DoS and multifractal scaling consistent with the conformal field theory (CFT) SO(), where counts replicas. This is contrary to the naive expectation of a surface thermal metal, and implies that the topology tunes the surface renormalization group to the CFT in the presence of disorder.
Published Version in PRB (Editors' Suggestion): 49 Pages, 17 Figures, 3 Tables
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