Vanishing edge currents in non--wave topological chiral superconductors
arXiv:1410.0377 · doi:10.1103/PhysRevB.90.224519
Abstract
The edge currents of two dimensional topological chiral superconductors with nonzero Cooper pair angular momentum---e.g., chiral -, -, and -wave superconductivity---are studied. Bogoliubov-de Gennes and Ginzburg--Landau calculations are used to show that in the continuum limit, \emph{only} chiral -wave states have a nonzero edge current. Outside this limit, when lattice effects become important, edge currents in non--wave superconductors are comparatively smaller, but can be nonzero. Using Ginzburg--Landau theory, a simple criterion is derived for when edge currents vanish for non--wave chiral superconductivity on a lattice. The implications of our results for putative chiral superconductors such as Sr2RuO4 and UPt3 are discussed.
9 pages, 5 figures. Published version
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Cited by in corpus (12)
- Topological surface states in nodal superconductors
- Orbital Angular Momentum and Spectral Flow in Two Dimensional Chiral Superfluids
- Non-topological nature of the edge current in a chiral p-wave superconductor
- Effective theory of two-dimensional chiral superfluids: gauge duality and Newton-Cartan formulation
- Orbital momentum of chiral superfluids and spectral asymmetry of edge states
- Surface magnetism in a chiral d-wave superconductor with hexagonal symmetry
- Orbital angular momentum in a nonchiral topological superconductor
- A review of some new perspectives on the theory of superconducting SrRuO
- Enhanced chiral edge currents and orbital magnetic moment in chiral -wave superconductors from mesoscopic finite-size effects
- Interband interference effects at the edge of a multiband chiral p-wave superconductor
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