Chiral Superconductivity in Thin Films of doped BiSe
arXiv:1801.02355 · doi:10.1103/PhysRevB.98.014505
Abstract
Recent experimental evidences point to rotation symmetry breaking superconductivity in doped BiSe, where the relevant order parameter belongs to a two-component odd-parity representation of the crystal point group. The channel admits two possible phases, the chiral phase, that breaks time-reversal symmetry, and nematic phase, that well explains the reported rotation symmetry breaking. In weakly anisotropic three-dimensional systems the nematic phase is the stable one. We study the stability of the nematic phase versus the chiral phase as a function of the anisotropy of the system and the thickness of the sample and show that in the strongly anisotropic case or in thin slabs the chiral phases is favoured. For the extreme 2D limit composed by a single layer of BiSe the system hosts two chiral Majorana modes flowing at the boundary of the system.
6 pages, 3 figures
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- Symmetries, Length Scales, Magnetic Response and Skyrmion Chains in Nematic Superconductors
- Spontaneous strain and magnetization in doped topological insulators with nematic and chiral superconductivity
- The absence of Ginzburg-Landau mechanism for vestigial order in the normal phase above a two-component superconductor
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- Surface chiral superconductivity in odd-parity nematic superconductors with magnetic impurities
- Anomalous Josephson Hall effect in doped topological insulators with the nematic superconductivity