J. Phys. Soc. Jpn. 77 (2008) Supplement C pp. 96-98  |Previous Article| |Next Article|  |Table of Contents|
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Proc. Int. Symp. Fe-Pnictide Superconductors

Unconventional Superconductivity Originating from Disconnected Fermi Surfaces in the Iron-Based Oxypnictide

Kazuhiko Kuroki1, Seiichiro Onari2, Ryotaro Arita3, Hidetomo Usui1, Yukio Tanaka2, Hiroshi Kontani4, and Hideo Aoki5

1Department of Applied Physics and Chemistry, The University of Electro-Communications, Chofu, Tokyo 182-8585
2Department of Applied Physics, Nagoya University, Nagoya 464-8603 and CREST-JST
3Department of Applied Physics, University of Tokyo, Tokyo 113-8656
4Department of Physics, Nagoya University, Nagoya 464-8602
5Department of Physics, University of Tokyo, Tokyo 113-0033

(Received August 4, 2008)

For a newly discovered iron-based high Tc superconductor LaFeAsO1-xFx, we have first constructed a minimal model, where all of the five Fe d bands turn out to be involved. We then investigate the origin of superconductivity with a five-band random-phase approximation by solving the Eliashberg equation. We conclude that the spin fluctuation modes arising from the nesting across the disconnected Fermi pockets realize an extended s-wave pairing, where, to be precise, the gap function is a 5×5 matrix.

URL: http://jpsj.ipap.jp/link?JPSJS/77SC/96/


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References

  1. Y. Kamihara et al.: J. Am. Chem. Soc. 130 (2008) 3296[CrossRef].
  2. K. Kuroki, S. Onari, R. Arita, H. Usui, Y. Tanaka, H. Kontani, and H. Aoki: Phys. Rev. Lett. 101 (2008) 087004[APS].
  3. H. Aoki: Physica C 437–438 (2006) 11[CrossRef]; H. Aoki: in Condensed Matter Theories, ed. H. Akai et al. (Nova Science, 2007) Vol. 21.
  4. C. de la Cruz et al.: Nature 453 (2008) 899[CrossRef].
  5. S. Baroni et al.: http://www.pwscf.org/. Here we adopt the exchange correlation functional introduced by J. P. Perdew et al. [Phys. Rev. B 54 (1996) 16533[APS]], and the wave functions are expanded by plane waves up to a cutoff energy of 40 Ry. 103 k-point meshes are used with the special points technique by H. J. Monkhorst and J. D. Pack [Phys. Rev. B 13 (1976) 5188[APS]].
  6. D. J. Singh and M.-H. Du: Phys. Rev. Lett. 100 (2008) 237003[APS].
  7. N. Marzari and D. Vanderbilt: Phys. Rev. B 56 (1997) 12847[APS]; I. Souza et al.: Phys. Rev. B 65 (2002) 035109[APS]. The Wannier functions are generated by the code developed by A. A. Mostofi et al. (http://www.wannier.org/) for the energy window -2 eV<εk-EF<2.6 eV, where εk is the eigenenergy of the Bloch states and EF the Fermi energy.
  8. While an ambiguity exists in unfolding the BZ [if the sign of the hoppings txy;µ, ν) with Δxy=odd (i.e., hoppings between A and B sites in a bipartite lattice) is changed, a band structure is reflected with respect to |kx|+|ky|=π], this is just a unitary transformation, and either way the five-band structure gives the same ten bands in the folded BZ as well as the same RPA results.
  9. K. Yada and H. Kontani: J. Phys. Soc. Jpn. 74 (2005) 2161[IPAP].
  10. T. Takimoto et al.: Phys. Rev. B 69 (2004) 104504[APS].
  11. N. Bulut et al.: Phys. Rev. B 45 (1992) 5577[APS].
  12. K. Kuroki and R. Arita: Phys. Rev. B 64 (2001) 024501[APS].
  13. K. Kuroki et al.: Phys. Rev. B 66 (2002) 184508[APS].
  14. K. Takada: Nature 422 (2003) 53[CrossRef].
  15. K. Kuroki et al.: Phys. Rev. B 73 (2006) 184503[APS].
  16. I. I. Mazin, D. J. Singh, M. D. Johannes, and M. H. Du: Phys. Rev. Lett. 101 (2008) 057003[APS].

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