4.6 Article

Impurity effects on the ±s-wave state of the iron-based superconductors

Journal

PHYSICAL REVIEW B
Volume 79, Issue 5, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.79.054529

Keywords

arsenic compounds; d-wave superconductivity; electronic density of states; impurity scattering; iron compounds; magnetic impurities; nuclear spin-lattice relaxation; photoelectron spectra; superconducting energy gap; superconducting materials; superconducting transition temperature; tunnelling spectra

Funding

  1. KOSEF [KRF-2007-521-C00081, KRF-2007-070-C00044]
  2. Basic Research Program [R01-2006-000-11248-0]
  3. Hallym University Research [HRF-2007-030]
  4. National Research Foundation of Korea [AA, 313-2008-2-C00241, 과06B1110, 2005-070-C00044] Funding Source: Korea Institute of Science & Technology Information (KISTI), National Science & Technology Information Service (NTIS)

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We studied the impurity scattering on the +/- s-wave superconductor (SC), with realistic parameters for the Fe pnictide SCs. Using the T-matrix method, generalized for the two bands, we found that the strong scattering limit of impurities forms an off-centered resonance state inside the superconducting (SC) gap, which modifies, surprisingly, the density of states (DOS) of a fully opened gap to a V-shaped DOS as if in the case of a d-wave SC. This behavior provides coherent explanations to the several conflicting experiments of the Fe-based SC: (1) the V-shaped DOS observed in photoemission and tunneling spectroscopy but with an isotropic gap; (2) the power-law behavior of the nuclear-spin-lattice relaxation rate (1/T(1)similar to T(alpha) with alpha similar to 3) down to very low temperatures. We also extended the same T-matrix method to study the impurity suppression of the critical temperature T(c) of the +/- s-wave pairing state. We found that both magnetic and nonmagnetic impurities suppress T(c) with a rate that is practically indistinguishable from the standard d-wave case despite a possibly large difference of the positive and the negative s-wave order parameter magnitudes.

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