Orbitally driven spin-singlet dimerization in S = 1 La4Ru2O10
Hua Wu,1 Zhiwei Hu,1 Tobias Burnus,1 Jonathan D. Denlinger,2 Peter G. Khalifah,3,4 David G. Mandrus,4 Ling-Yun Jang,5 Hui Huang Hsieh,6 Arata Tanaka,7 Keng S. Liang,5 Jim W. Allen,8 Robert J. Cava,9 Daniel I. Khomskii1 and L. Hao Tjeng1
1 II. Physikalisches Institut, Universität zu Köln, Zülpicher Str. 77, 50937 Köln, Germany
2 Advanced Light Source, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
3 Department of Chemistry, University of Massachusetts, Amherst, MA 01003, USA
4 Condensed Matter Sciences Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831, USA
5 National Synchrotron Radiation Research Center, 101 Hsin-Ann Road, Hsinchu 30077, Taiwan
6 Chung Cheng Institute of Technology, National Defense University, Taoyuan 335, Taiwan
7 Department of Quantum Matter, ADSM, Hiroshima University, Higashi-Hiroshima 739-8530, Japan
8 Randall Laboratory of Physics, University of Michigan, Ann Arbor, MI 48109, USA
9 Department of Chemistry, Princeton University, Princeton, NJ 08540, USA
[Abstract][References]
Abstract
Using x-ray absorption spectroscopy at the Ru-L2,3 edge we reveal that the Ru4+ ions remain in the S = 1 spin state across the rare 4d-orbital ordering transition and spin-gap formation. We find using local spin density approximation + Hubbard U (LSDA+U) band structure calculations that the crystal fields in the low temperature phase are not strong enough to stabilize the S = 0 state. Instead, we identify a distinct orbital ordering with a significant anisotropy of the antiferromagnetic exchange couplings. We conclude that La4Ru2O10 appears to be a novel material in which the orbital physics drives the formation of spin-singlet dimers in a quasi 2-dimensional S = 1 system.
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This article is cited by
(This list might be incomplete; order as found; as of 11 January 2007)
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