Home | About Journal | Web Links | E-mail Alerts | RSS RSS Icon | Browse
Previous Article Next Article

Bulk electronic structure of optimally doped Ba(Fe1−xCox)2As2

Source: Phys. Rev. B 81, 064509 (2010); doi:10.1103/PhysRevB.81.064509

Published 18 February 2010

PACS
  • 71.18.+y
    Fermi surface: calculations and measurements; effective mass, -g factor
  • 74.70.-b
    Superconducting materials
  • 78.70.Ck
    X-ray scattering (condensed matter)
  • YEAR: 2010
PUBLICATION DATA
Publisher:
AIP is a member of CrossRef APS
C. Utfeld,1 J. Laverock,1 T. D. Haynes,1 S. B. Dugdale,1 J. A. Duffy,2 M. W. Butchers,2 J. W. Taylor,3 S. R. Giblin,3 J. G. Analytis,4,5 J.-H. Chu,4,5 I. R. Fisher,4,5 M. Itou,6 and Y. Sakurai6
1H. H. Wills Physics Laboratory, University of Bristol, Tyndall Avenue, Bristol BS8 1TL, United Kingdom
2Department of Physics, University of Warwick, Coventry CV47AL, United Kingdom
3ISIS Facility, Rutherford Appleton Laboratory, Chilton, Oxfordshire OX11 0QX, United Kingdom
4Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA
5Geballe Laboratory for Advanced Materials and Department of Applied Physics, Stanford University, Stanford, California 94305, USA
6Japan Synchrotron Radiation Research Institute, SPring-8, 1-1-1 Kouto, Sayo, Hyogo 679-5198, Japan

We report high-resolution, bulk Compton scattering measurements unveiling the Fermi surface of an optimally doped iron-arsenide superconductor, Ba(Fe0.93Co0.07)2As2. Our measurements are in agreement with first-principles calculations of the electronic structure, revealing both the X-centered electron pockets and the Gamma-centered hole pockets. Moreover, our data are consistent with the strong three dimensionality of one of these sheets that has been predicted by electronic structure calculations at the local-density-approximation-minimum As position. Complementary calculations of the noninteracting susceptibility, chi0(q,omega), suggest that the broad peak that develops due to interband Fermi-surface nesting, and which has motivated several theories of superconductivity in this class of material, survives the measured three dimensionality of the Fermi surface in this family. ©2010 The American Physical Society
History: Received 15 January 2010; published 18 February 2010
Permalink: http://link.aps.org/abstract/PRB/v81/e064509
ADVERTISEMENT