Effect of the type I to type II Weyl semimetal topological transition on superconductivity
arXiv:1612.09048 · doi:10.1103/PhysRevB.95.094513
Abstract
The influence of recently discovered topological transition between type I and type II Weyl semi-metals on superconductivity is considered. A set of Gorkov equations for weak superconductivity in Weyl semi-metal under topological phase transition is derived and solved. The critical temperature and superconducting gap both have spike in the point the transition point as function of the tilt parameter of the Dirac cone determined in turn by the material parameters like pressure. The spectrum of superconducting excitations is different in two phases: the sharp cone pinnacle is characteristic for a type I, while two parallel almost flat bands, are formed in type II. Spectral density is calculated on both sides of transition demonstrate different weight of the bands. The superconductivity thus can be used as a clear indicator for the topological transformation. Results are discussed in the light of recent experiments.
13 pages, 5 figures
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- Control of superconducting pairing symmetries in monolayer black phosphorus
- Type-II Dirac states in full Heusler compounds XInPd2 (X = Ti, Zr and Hf)
- Type-III Dirac Cones from Degenerate Directionally Flat Bands: Viewpoint from Molecular-Orbital Representation
- Strong magnetic field induces superconductivity in Weyl semi - metal