Magnetic Intragap States and Mixed Parity Pairing at the Edge of Spin-Triplet Superconductors
arXiv:1210.8282 · doi:10.1103/PhysRevLett.110.267002
Abstract
We show that a spontaneous magnetic moment may appear at the edge of a spin-triplet superconductor if the system allows for pairing in a subdominant channel. To unveil the microscopic mechanism behind such effect we combine numerical solution of the Bogoliubov-De Gennes equations for a tight-binding model with nearest-neighbor attraction, and the symmetry based Ginzburg-Landau approach. We find that a potential barrier modulating the electronic density near the edge of the system leads to a non-unitary superconducting state close to the boundary where spin-singlet pairing coexists with the dominant triplet superconducting order. We demonstrate that the spin polarization at the edge appears due to the inhomogeneity of the non-unitary state and originates in the lifting of the spin-degeneracy of the Andreev bound-states.
5 pages, 3 figures and Supplemental material (2 pages)
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Cited by in corpus (7)
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- Topological signatures of the coexistence of antiferromagnetism and odd-parity spin-triplet superconductivity
- Control of magnetism in singlet-triplet superconducting heterostructures
- Interface currents and magnetization in singlet-triplet superconducting heterostructures: Role of chiral and helical domains
- Electron transport in p-wave superconductor-normal metal junctions
- Magnetic exchange interaction in spin-valve with chiral spin-triplet superconductor