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Phys. Rev. Lett. 102, 037205 (2009) [4 pages]

Magnetic Structure of RuSr2GdCu2O8 Determined by Resonant X-Ray Diffraction

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B. Bohnenbuck1, I. Zegkinoglou1, J. Strempfer2, C. S. Nelson3, H.-H. Wu4,5, C. Schüßler-Langeheine4, M. Reehuis1,6, E. Schierle6, Ph. Leininger1, T. Herrmannsdörfer7, J. C. Lang8, G. Srajer8, C. T. Lin1, and B. Keimer1
1Max-Planck-Institut für Festkörperforschung, Heisenbergstraße 1, 70569 Stuttgart, Germany
2Hamburger Synchrotronstrahlungslabor HASYLAB at DESY, Notkestraße 85, 22603 Hamburg, Germany
3National Synchrotron Light Source, Brookhaven National Laboratory, Upton, New York 11973-5000, USA
4Physikalisches Institut, Universität zu Köln, Zülpicher Straße 77, 50937 Köln, Germany
5National Synchrotron Radiation Research Center, Hsinchu 30076, Taiwan
6Helmholtz-Zentrum Berlin, Albert-Einstein-Straße 15, 12489 Berlin, Germany
7Hochfeld-Magnetlabor Dresden (HLD), Forschungszentrum Dresden-Rossendorf, 01314 Dresden, Germany
8Advanced Photon Source, Argonne National Laboratory, Argonne, Illinois 60439, USA

Received 22 October 2008; published 22 January 2009

X-ray diffraction with photon energies near the Ru L2-absorption edge was used to detect resonant reflections characteristic of a G-type superstructure in RuSr2GdCu2O8 single crystals. A polarization analysis confirms that these reflections are due to magnetic order of Ru moments, and the azimuthal-angle dependence of the scattering amplitude reveals that the moments lie along a low-symmetry axis with substantial components parallel and perpendicular to the RuO2 layers. Complemented by susceptibility data and a symmetry analysis of the magnetic structure, these results reconcile many of the apparently contradictory findings reported in the literature.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevLett.102.037205
DOI:
10.1103/PhysRevLett.102.037205
PACS:
75.30.−m, 75.25.+z, 75.50.Ee, 78.70.Ck