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Electronic theory for superconductivity in Sr2_2RuO4_4: triplet pairing due to spin-fluctuation exchange

Abstract

Using a two-dimensional Hubbard Hamiltonian for the three electronic bands crossing the Fermi level in Sr2_2RuO4_4 we calculate the band structure and spin susceptibility χ(q,ω)\chi({\bf q}, \omega) in quantitative agreement with nuclear magnetic resonance (NMR) and inelastic neutron scattering (INS) experiments. The susceptibility has two peaks at {\bf Q}i=(2π/3,2π/3)_i = (2\pi/3, 2\pi/3) due to the nesting Fermi surface properties and at {\bf q}i=(0.6π,0)_i = (0.6\pi, 0) due to the tendency towards ferromagnetism. Applying spin-fluctuation exchange theory as in layered cuprates we determine from χ(q,ω)\chi({\bf q}, \omega), electronic dispersions, and Fermi surface topology that superconductivity in Sr2_2RuO4_4 consists of triplet pairing. Combining the Fermi surface topology and the results for χ(q,ω)\chi({\bf q}, \omega) we can exclude ss- and dd-wave symmetry for the superconducting order parameter. Furthermore, within our analysis and approximations we find that ff-wave symmetry is slightly favored over p-wave symmetry due to the nesting properties of the Fermi surface.Comment: 5 pages, 5 figures, misprints correcte

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    Last time updated on 01/04/2019