Triplet superconductivity in 3D Dirac semimetal due to exchange interaction
arXiv:1407.0770 · doi:10.1088/0953-8984/27/2/025701
Abstract
Conventional phonon-electron interaction induces either triplet or one of two (degenerate) singlet pairing states in time reversal and inversion invariant 3D Dirac semi - metal. Investigation of the order parameters and energies of these states at zero temperature in wide range of values of chemical potential , the effective electron-electron coupling constant and Debye energy demonstrates that when the exchange interaction is neglected the singlet always prevails, however in significant portions of the parameter space the energy difference is very small. This means that interactions that are small but discriminate between the spin singlet and the spin triplet are important in order to determine the nature of the superconducting order there. The best candidate for such an interaction in materials under consideration is the exchange (the Stoner term) characterized by constant . We show that at values of much smaller then ones creating Stoner instability to ferromagnetism the triplet pairing becomes energetically favored over the singlet ones for % . The 3D quantum critical point at is considered in detail.
13 pages, 11 figures
References in corpus (10)
- Bulk Band Gap and Surface State Conduction Observed in Voltage-Tuned Crystals of the Topological Insulator BiSe
- Electron-phonon Coupling on the Surface of the Topological Insulator Bi2Se3: Determined from Surface Phonon Dispersion Measurements
- Time-reversal invariant topological superconductivity in doped Weyl semimetals
- Topological Weyl Semi-metal from a Lattice Model
- Quantum superconducting criticality in graphene and topological insulators
- Low-Energy Effective Hamiltonian and the Surface States of Ca_3PbO
- Relativistic quantum effects of Dirac particles simulated by ultracold atoms
- Interband Effects of Magnetic Field on Hall Effects for Dirac Electrons in Bismuth
- Pairing symmetry and vortex zero-mode for superconducting Dirac fermions
- Quantum critical point in the superconducting transition on the surface of topological insulator