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Phys. Rev. B 69, 134419 (2004) [16 pages]

Resonant x-ray diffraction of the magnetoresistant perovskite Pr0.6Ca0.4MnO3

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S. Grenier1,2, J. P. Hill2, Doon Gibbs2, K. J. Thomas2, M. v. Zimmermann3, C. S. Nelson4, V. Kiryukhin1, Y. Tokura5, Y. Tomioka5, D. Casa6, T. Gog6, and C. Venkataraman6
1Department of Physics and Astronomy, Rutgers University, Piscataway, New Jersey 08854, USA
2Department of Physics, Brookhaven National Laboratory, Upton, New York 11973, USA
3Hamburger Synchrotronstrahlungslabor (HASYLAB) at Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, 22603 Hamburg, Germany
4NRL-SRC, NSLS, Brookhaven National Laboratory, Upton, New York, 11973, USA
5Joint Research Center for Atom Technology (JRCAT), Tsukuba 305-0046, Japan
6CMC-CAT, Advanced Photon Source, Argonne National Laboratory, Argonne, Illinois 60439, USA

Received 8 May 2003; revised 21 October 2003; published 15 April 2004

We report a resonant x-ray-diffraction study of the magnetoresistant perovskite Pr0.6Ca0.4MnO3. We discuss the spectra measured above and below the semiconductor-insulator transition temperature with the aid of a detailed formal analysis of the energy and polarization dependences of the structure factors and ab initio calculations of the spectra. In the low-temperature insulating phase, we find that inequivalent Mn atoms order in a CE-type pattern and that the crystallographic structure of La0.5Ca0.5MnO3 [Radaelli et al., Phys. Rev. B 55, 3015 (1997)] can also describe this system in detail. Instead, the alternative structure proposed for the so-called Zener-polaron model [Daoud-Aladine et al., Phys. Rev. Lett. 89, 097205 (2002)] is ruled out by crystallographic and spectroscopic evidence. Our analysis supports a model involving orbital ordering. However, we confirm that there is no direct evidence of charge disproportionation in the Mn K-edge resonant spectra. Therefore, we consider a CE-type model in which there are two Mn sublattices, each with partial eg occupancy. One sublattice consists of Mn atoms with the 3x2-r2 or 3y2-r2 orbitals partially occupied in an alternating pattern, the other sublattice with the x2-y2 orbital partially occupied.

© 2004 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.69.134419
DOI:
10.1103/PhysRevB.69.134419
PACS:
75.47.Lx, 75.47.Gk, 61.10.Nz, 61.10.Ht