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Local structure of the superconductor K0.8Fe1.6+xSe2: Evidence of large structural disorder

Source: Phys. Rev. B 85, 024504 (2012); http://dx.doi.org/10.1103/PhysRevB.85.024504

Published 3 January 2012

PACS
  • 74.70.-b
    Superconducting materials
  • 78.70.Dm
    X-ray absorption spectra (condensed matter)
  • 61.05.cj
    X-ray absorption spectroscopy (condensed matter structure determination)
  • YEAR: 2011
PUBLICATION DATA
Publisher:
AIP is a member of CrossRef APS
T. A. Tyson,1 T. Yu,1 S. J. Han,2 M. Croft,3 G. D. Gu,2 I. K. Dimitrov,2 and Q. Li2
1Department of Physics, New Jersey Institute of Technology, Newark, New Jersey 07102, USA
2Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton New York 11973, USA
3Department of Physics and Astronomy, Rutgers University, Piscataway, New Jersey 08854, USA

The local structure of superconducting single crystals of K0.8Fe1.6+xSe2 with Tc = 32.6 K was studied by x-ray absorption spectroscopy. Near-edge spectra reveal that the average valence of Fe is 2+. The room temperature structure about the Fe, K, and Se sites was examined by iron, selenium, and potassium K-edge measurements. The structure about the Se and Fe sites shows a high degree of order in the nearest-neighbor Fe-Se bonds. On the other hand, the combined Se and K local structure measurements reveal a very high level of structural disorder in the K layers. Temperature-dependent measurements at the Fe sites show that the Fe-Se atomic correlation follows that of the Fe-As correlation in the superconductor LaFeAsO0.89F0.11, having the same effective Einstein temperature (stiffness). In K0.8Fe1.6+xSe2, the nearest-neighbor Fe-Fe bonds have a lower Einstein temperature and higher structural disorder than in LaFeAsO0.89F0.11. The moderate Fe site and high K site structural disorder is consistent with the high normal state resistivity seen in this class of materials. For higher shells, an enhancement of the second-nearest-neighbor Fe-Fe correlation is found just below Tc, possibly due to changes in magnetic or local structural ordering.
History: Received 4 November 2011; revised 13 December 2011; published 3 January 2012
Digital Object Identifier: http://dx.doi.org/10.1103/PhysRevB.85.024504
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