Theory of low-energy behaviors in topological $s$-wave pairing superconductors

We construct a low-energy effective theory of topological $s$-wave pairing superconductors, focusing on the mean-field model of superconductor $C{u}_{x}B{i}_{2}S{e}_3$. 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 $B{i}_{2}S{e}_3$. 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 $p$-wave-like component as the primary contribution, but also an $s$-wave-like one as higher-order corrections. The mixture of $p$- and $s$-wave explains the numerical results [Phys. Rev. B 89 (2014) 214506] of the non-magnetic impurity effects.