High- superconductivity by mobilizing local spin singlets and possible route to higher in pressurized LaNiO
arXiv:2308.09044 · doi:10.1103/PhysRevB.108.L140504
Abstract
We clarify the pairing mechanism of high- superconductivity in bilayer LaNiO under high pressure by employing the static auxiliary field Monte Carlo approach to simulate a minimal effective model that contains local interlayer spin singlets and metallic bands. Superconductivity is induced when the local spin singlet pairs are mobilized and attain long-distance phase coherence by hybridization with the metallic bands. When projected onto realistic Fermi surfaces, it yields a nodeless -wave gap on the Fermi surface, and extended -wave gaps of the same (opposite) sign on the () Fermi surface due to its bonding (antibonding) character, with nodes or gap minima along the diagonal direction of the two-dimensional Brillouin zone. We find a dual role of the hybridization that not only induces global phase coherence but also competes with the spin singlet formation. This lead to a tentative phase diagram where varies nonmonotonically with the hybridization, in good correspondence with experimental observations. A roughly linear relation is obtained for realistic hopping and hybridization parameters: , where is the interlayer superexchange interaction. We emphasize the peculiar tunability of the bilayer structure and propose that may be further enhanced by hole doping or applying uniaxial pressure along the axis on superconducting LaNiO. Our work provides reliable numerical evidence for the pairing mechanism of high- superconductivity in LaNiO and points out a potential route to achieve even higher .
7 pages,4 figures
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