Two-dimensional topological superconducting phases emerged from d-wave superconductors in proximity to antiferromagnets
arXiv:1610.08728 · doi:10.1209/0295-5075/118/37004
Abstract
Motivated by the recent observations of nodeless superconductivity in the monolayer CuO grown on the BiSrCaCuO substrates, we study the two-dimensional superconducting (SC) phases described by the two-dimensional - model in proximity to an antiferromagnetic (AF) insulator. We found that (i) the nodal d-wave SC state can be driven via a continuous transition into a nodeless d-wave pairing state by the proximity induced AF field. (ii) The energetically favorable pairing states in the strong field regime have extended s-wave symmetry and can be nodal or nodeless. (iii) Between the pure d-wave and s-wave paired phases, there emerge two topologically distinct SC phases with (i) symmetry, i.e., the weak and strong pairing phases, and the weak pairing phase is found to be a topological superconductor protected by valley symmetry, exhibiting robust gapless non-chiral edge modes. These findings strongly suggest that the high- superconductors in proximity to antiferromagnets can realize fully gapped symmetry protected topological SC.
7 pages, 4 figures; revised version
References in corpus (4)
- Classification of topological insulators and superconductors in three spatial dimensions
- Nodeless pairing in superconducting copper-oxide monolayer films on Bi2Sr2CaCu2O8+δ
- Marginality of bulk-edge correspondence for single-valley Hamiltonians
- Stability of nodal quasi-particles in superconductors with coexisting orders
Cited by in corpus (5)
- Superconductivity in a unique type of copper oxide
- Nodeless high-T superconductivity in highly-overdoped monolayer CuO
- Antiferromagnetism-driven two-dimensional topological nodal-point superconductivity
- Superconducting dome with - pairing symmetry in the heavily hole-overdoped copper-oxide planes
- Symmetry-dependent antiferromagnetic proximity effects on valley splitting