Theory of low-energy behaviors in topological -wave pairing superconductors
arXiv:1510.06910 · doi:10.1016/j.physc.2015.08.002
Abstract
We construct a low-energy effective theory of topological -wave pairing superconductors, focusing on the mean-field model of superconductor $\mbox{Cu}_{x}\mbox{Bi}_{2}\mbox{Se}_{3}$. Our approach is second-order perturbation with respect to the inverse of the mass (i.e., large-mass expansion) in the Dirac-type electron dispersion from topological insulator $\mbox{Bi}_{2}\mbox{Se}_{3}$. Since the Dirac-type dispersion with a large mass describes non-relativistic electrons, the large-mass expansion corresponds to a low-energy theory with respect to the original setup. We show that the effective gap function has not only a -wave-like component as the primary contribution, but also an -wave-like one as higher-order corrections. The mixture of - and -wave explains the numerical results [Phys. Rev. B 89 (2014) 214506] of the non-magnetic impurity effects.
Proceedings of 27th International Symposium on Superconductivity (ISS2014). Comments are welcome
References in corpus (7)
- Local Measurements of the Superconducting Pairing Symmetry in CuxBi2Se3
- Surface spectral function in the superconducting state of a topological insulator
- A new superconductor derived from topological insulator heterostructure
- Dirac-Fermion-Induced Parity Mixing in Superconducting Topological Insulators
- Non-fragile superconductivity with nodes in the superconducting topological insulator CuxBi2Se3: Zeeman orbital field and non-magnetic impurities
- Non-magnetic impurity effects in a three-dimensional topological superconductor: From p- to s-wave behaviors
- Effective low energy theory for surface Andreev bound states of superconducting phases in generalized Bernevig-Hughes-Zhang models