Mechanism for the Singlet to Triplet Superconductivity Crossover in Quasi-One-Dimensional Organic Conductors
arXiv:0906.2285 · doi:10.1143/JPSJ.78.104702
Abstract
Superconductivity of quasi-one-dimensional organic conductors with a quarter-filled band is investigated using the two-loop renormalization group approach to the extended Hubbard model for which both the single electron hopping t_{\perp} and the repulsive interaction V_{\perp} perpendicular to the chains are included. For a four-patches Fermi surface with deviations to perfect nesting, we calculate the response functions for the dominant fluctuations and possible superconducting states. By increasing V_{\perp}, it is shown that a d-wave (singlet) to f-wave (triplet) superconducting state crossover occurs, and is followed by a vanishing spin gap. Furthermore, we study the influence of a magnetic field through the Zeeman coupling, from which a triplet superconducting state is found to emerge.
11 pages, 15 figures, published version
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Cited by in corpus (5)
- Emergence of Charge Loop Current in Geometrically Frustrated Hubbard Model: Functional Renormalization Group Study
- On the Origin of the Anomalous Upper Critical Field in Quasi-One-Dimensional Superconductors
- - and -wave quantum liquid crystal orders in cuprate superconductors, -(BEDT-TTF)X, and coupled chain Hubbard models: functional-renormalization-group analysis
- Microscopic theory of a superconducting gap in the quasi-one-dimensional organic conductor (TMTSF)ClO: Model derivation and two-particle self-consistent analysis
- Superconducting and density-wave instabilities of low dimensional conductors with a Zeeman coupling to a magnetic field