Coexistence of magnetism and superconductivity in a t-J bilayer
arXiv:0710.2638 · doi:10.1103/PhysRevB.76.235122
Abstract
We investigate coexistence of antiferromagnetic and superconducting correlations in bilayered materials using a two-dimensional t-J model with couplings across the layers using variational Monte Carlo calculations. It is found that the underdoped regime supports a coexisting phase, beyond which the (d-wave) superconducting state becomes stable. Further, the effects of interplanar coupling parameters on the magnetic and superconducting correlations as a function of hole doping are studied in details. The magnetic correlations are found to diminish with increasing interplanar hopping away from half filling, while the exchange across the layers strengthens interplanar antiferromagnetic correlations both at and away from half filling. The superconducting correlations show more interesting features where larger interplanar hopping considerably reduces planar correlations at optimal doping, while an opposite behaviour, i.e. stabilisation of the superconducting state is realised in the overdoped regime, with the interplanar exchange all the while playing a dormant role.
arXiv comment8 pages, 9 figures, RevTex4, Submitted to Phys. Rev. B
References in corpus (10)
- SO(5) Theory of Antiferromagnetism and Superconductivity
- Incommensurate Magnetic Fluctuations in YBa2Cu3O6.6
- High Tc Superconductors -- A Variational Theory of the Superconducting State
- Phase Diagram and Pairing Symmetry of the Two-Dimensional t-J Model by a Variation Theory
- Neutron scattering and superconducting order parameter in YBa2Cu3O7
- Coexistence of Superconductivity and Antiferromagnetism in Multilayered High- Superconductor HgBaCaCuO: A Cu-NMR Study
- Magnetic excitations and their anisotropy in YBCO: slave-boson mean-field analysis of bilayer t-J model
- s-wave superconductivity from antiferromagnetic spin-fluctuation model for bilayer materials
- Ground state properties and dynamics of the bilayer t-J model
- Antiferromagnetic Interactions and the Superconducting Gap Function