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Phys. Rev. B 65, 214413 (2002) [12 pages]

High-magnetic-field NMR studies of LiVGe2O6: A quasi-one-dimensional spin S=1 system

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P. Vonlanthen1, K. B. Tanaka1, Atsushi Goto1,2, W. G. Clark1, P. Millet3, J. Y. Henry4, J. L. Gavilano5, H. R. Ott5, F. Mila6, C. Berthier7, M. Horvatic7, Yo Tokunaga7, P. Kuhns8, A. P. Reyes8, and W. G. Moulton8
1Department of Physics and Astronomy, University of California at Los Angeles, Los Angeles, California 90095-1547
2National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan
3Centre d’Elaboration des Matériaux et d’Etudes Structurales, 29 rue J. Marvig, 31055 Toulouse Cedex, France
4Centre d’Etudes Nucléaires, DRFMC/SPSMS/MDN, F-38054 Grenoble Cedex 9, France
5Laboratorium für Festkörperphysik, ETH-Hönggerberg, CH-8093 Zürich, Switzerland
6Institut de Physique Théorique, Université de Lausanne, 1015 Lausanne, Switzerland
7Grenoble High Magnetic Field Laboratory, BP 166, 38042 Grenoble Cedex 9, France
8National High Magnetic Field Laboratory, Tallahassee, Florida 32310

Received 10 December 2001; published 29 May 2002

We report 7Li pulsed NMR measurements in polycrystalline and single-crystal samples of the quasi-one-dimensional S=1 antiferromagnet LiVGe2O6, whose AF transition temperature is TN24.5K. The field (B0) and temperature (T) ranges covered were 9–44.5 T and 1.7–300 K, respectively. The measurements included NMR spectra, the spin-lattice relaxation rate (T1-1), and the spin-phase relaxation rate (T2-1), often as a function of the orientation of the field relative to the crystal axes. The spectra indicate an AF magnetic structure consistent with that obtained from neutron diffraction measurements, but with the moments aligned parallel to the c axis. The spectra also provide the T-dependence of the AF order parameter and show that the transition is either second-order or weakly first-order. Both the spectra and the T1-1 data show that B0 has at most a small effect on the alignment of the AF moment. There is no spin-flop transition up to 44.5 T. These features indicate a very large magnetic anisotropy energy in LiVGe2O6, with orbital degrees of freedom playing an important role. Below 8 K, T1-1 varies substantially with the orientation of B0 in the plane perpendicular to the c axis, suggesting a small energy gap for magnetic fluctuations that is very anisotropic.

© 2002 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.65.214413
DOI:
10.1103/PhysRevB.65.214413
PACS:
75.30.Kz, 75.50.Ee, 76.60.-k