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Phys. Rev. B 82, 024421 (2010) [5 pages]

Magnetization distribution in the tetragonal phase of BaFe2As2

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P. J. Brown1,2, T. Chatterji3, A. Stunault1, Y. Su4, Y. Xiao5, R. Mittal4,6, Th. Brückel4,5, Th. Wolf7, and P. Adelmann7
1Institut Laue-Langevin, BP 156, 38042 Grenoble Cedex 9, France
2Department of Physics, Loughborough University, Loughborough LE11 3TU, United Kingdom
3JCNS, Forschungszentrum Jülich, Outstation at Institut Laue-Langevin, BP 156, 38042 Grenoble Cedex 9, France
4JCNS, Forschungszentrum Jülich, Outstation at FRM II, Lichtenbergstrasse 1, 85747 Garching, Germany
5Institut für Feskörperforschung, Forschungzentrum Jülich, 52425 Jülich, Germany
6Solid State Physics Division, Bhabha Atomic Research Centre, Trombay, Mumbai 400085, India
7Karlsruhe Institute of Technology, Institut fuer Festkoerperphysik, D-76021 Karlsruhe, Germany

Received 4 June 2010; revised 6 July 2010; published 21 July 2010

We have determined the spatial distribution of the magnetization induced by a field of 9 T in the tetragonal phase of BaFe2As2 using polarized neutron diffraction. Magnetic structure factors derived from the polarization dependence of the intensities of Bragg reflections were used to make a maximum-entropy reconstruction of the distribution projected on the 110 plane. The reconstruction shows clearly that the magnetization is confined to the region around the iron atoms and that there is no significant magnetization associated with either As or Ba atoms. The distribution of magnetization around the Fe atom is significantly nonspherical with a shape which is extended in the ⟨111⟩ directions in the projection. These results show that the electrons which give rise to the paramagnetic susceptibility are confined to the Fe atoms their distribution suggests that they occupy 3d t2g-type orbitals with ≈60% in those of xy symmetry.

© 2010 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.82.024421
DOI:
10.1103/PhysRevB.82.024421
PACS:
75.25.-j