Antiferromagnetic Interactions and the Superconducting Gap Function
arXiv:cond-mat/9507013 · doi:10.1103/PhysRevB.53.5137
Abstract
Spin-fluctuation-mediated superconductivity is conventionally associated with d_{x^2-y^2} pairing. We show that a generalized model of antiferromagnetic spin fluctuations in three dimensions may also yield a state with formal ``s-wave'' (A_{1g}) symmetry but with line nodes at k_z \approx \pm π/ 2c. We study this new state within both BCS and Eliashberg theories using a realistic band structure and find that it is more stable than the d_{x^2-y^2} (B_{1g}) state over a wide range of parameters. Thus, models of spin-fluctuation-mediated superconductivity must consider both possibilities on an equal footing.
4 pages, RevTeX with psfig, 2 PostScript figures included in compressed form, one color PostScript figure available by request to [email protected] or [email protected]. Minor changes and updated references from original posting
References in corpus (2)
Cited by in corpus (5)
- A Survey of the Van Hove Scenario for High-T_c Superconductivity With Special Emphasis on Pseudogaps and Striped Phases
- Edge states and determination of pairing symmetry in superconducting Sr2RuO4
- Hole Dispersion and Symmetry of the Superconducting Order Parameter for Underdoped CuO Bilayers and 3D Antiferromagnets
- Theory for the Interdependence of High-T Superconductivity and Dynamical Spin Fluctuations
- Coexistence of magnetism and superconductivity in a t-J bilayer