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Phys. Rev. B 73, 184503 (2006) [6 pages]

Extended s-wave pairing originating from the a1g band in NaxCoO2·yH2O: Single-band U-V model with fluctuation exchange method

Kazuhiko Kuroki,1 Seiichiro Onari,2 Yukio Tanaka,2 Ryotaro Arita,3,4 and Takumi Nojima1
1Department of Applied Physics and Chemistry, The University of Electro-Communications, Chofu, Tokyo 182-8585, Japan
2Department of Applied Physics, Nagoya University, Nagoya, 464-8603, Japan
3Max Planck Institute for Solid State Research, Heisenbergstrasse 1, Stuttgart 70569, Germany
4Department of Physics, University of Tokyo, Hongo 7-3-1, Tokyo 113-0033, Japan

Received 24 February 2006; published 2 May 2006

Motivated by recent experiments and band calculation results, we investigate the possibility of superconductivity originating from the a1g band of NaxCoO2·yH2O assuming the absence of e<sub>g</sub><sup>[prime]</sup> pockets. We adopt a single band U-V model that takes into account the local minimum of the a1g band dispersion at the Gamma point. Using the fluctuation exchange method, we find that an unconventional s-wave pairing with a gap that changes sign between the inner and the outer Fermi surfaces is enhanced due to the coexistence of spin fluctuations at wave vectors bridging the two Fermi surfaces and the charge fluctuations near the K point. Possible relevance to the experimental results is discussed.

©2006 The American Physical Society

URL: http://link.aps.org/doi/10.1103/PhysRevB.73.184503
DOI: 10.1103/PhysRevB.73.184503
PACS: 74.20.Mn; 71.10.Fd; 74.20.Rp; 74.25.Ha
  • 74.20.Mn
    Nonconventional mechanisms of superconductivity including spin fluctuations, polarons and bipolarons, resonating valence bond model, anyon mechanism, marginal Fermi liquid, Luttinger liquid, etc
  • 71.10.Fd
    Lattice fermion models (condensed matter) including Hubbard model, etc
  • 74.20.Rp
    Pairing symmetries (other than s-wave) in superconductivity theory
  • 74.25.Ha
    Magnetic properties of superconductors
  • YEAR: 2006
KEYWORDS: sodium compounds, type II superconductors, superconducting energy gap, spin fluctuations, Fermi surface

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