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Structural precursor to the metal-insulator transition in V{sub 2}O{sub 3}

The temperature dependence of the local structure of V{sub 2}O{sub 3} in the vicinity of the metal-to-insulator transition (MIT) has been investigated using hard x-ray absorption spectroscopy. It is shown that the vanadium pair distance along the hexagonal c axis changes abruptly at the MIT as expec...

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Published in:Physical review. B, Condensed matter and materials physics Condensed matter and materials physics, 2006-04, Vol.73 (14)
Main Authors: Pfalzer, P., Obermeier, G., Klemm, M., Horn, S., Boer, M. L. den, Queens College of CUNY, 65-30 Kissena Boulevard, Flushing, New York 11367
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container_title Physical review. B, Condensed matter and materials physics
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creator Pfalzer, P.
Obermeier, G.
Klemm, M.
Horn, S.
Boer, M. L. den
Queens College of CUNY, 65-30 Kissena Boulevard, Flushing, New York 11367
description The temperature dependence of the local structure of V{sub 2}O{sub 3} in the vicinity of the metal-to-insulator transition (MIT) has been investigated using hard x-ray absorption spectroscopy. It is shown that the vanadium pair distance along the hexagonal c axis changes abruptly at the MIT as expected. However, a continuous increase of the tilt of these pairs sets in already at higher temperatures and reaches its maximum value at the onset of the electronic and magnetic transition. These findings confirm recent theoretical results which claim that electron-lattice coupling is important for the MIT in V{sub 2}O{sub 3}. Our results suggest that the distortion of the symmetry of the basal plane plays a decisive role for the MIT and orbital degrees of freedom drive the MIT via changes in hybridization.
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subjects ABSORPTION SPECTROSCOPY
CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY
COUPLING
DEGREES OF FREEDOM
DISTANCE
ELECTRONS
HARD X RADIATION
PHASE TRANSFORMATIONS
PRECURSOR
SYMMETRY
TEMPERATURE DEPENDENCE
VANADIUM
VANADIUM OXIDES
X-RAY SPECTRA
title Structural precursor to the metal-insulator transition in V{sub 2}O{sub 3}
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