W0265
Low Temperature Structural Changes in K2V3O8. B.C.
Chakoumakos1, K. Oikawa2, T. Kamiyama2, B.C.
Sales1, M.D. Lumsden1, S.E. Nagler1,
1Oak Ridge National Laboratory*, Oak Ridge, TN 37831-6393, USA,
2Inst. of Materials Structure Science, High Energy Accelerator
Research Organization, Tsukuba 305-0810 Japan.
The title compound has the fresnoite-type structure, which is
of interest because of unusual low temperature magnetic properties. K2V3O8 is a
two-dimensional S = 1/2 antiferromagnet (TN ~ 4K) that exhibits field-induced
spin reorientation [1] and enhancement of heat transport [2]. At 110K infrared,
permittivity, and heat capacity measurements [3] indicate a structural
distortion occurs, which may involve a change in the coordination geometry of
the magnetic V+4 ion. To better understand the details of the structural changes
occurring below110K and how they might impact the interpretation of the magnetic
field induced changes at lower temperature, we undertook neutron powder
diffraction measurements at 5, 10, 15, 20, 30, 40, 70, 100, 110, 130, 170, 200,
230, 270, and 295K on the time-of-flight instrument Vega at the high energy
accelerator research organization (KEK). For refinements made in the nominal
space group P4bm, the most dramatic change in the structure is evidenced by the
a cell edge, which expands initially on cooling, then abruptly begins to
contract at 110K. The c cell edge contracts monotonically. The atomic
displacement parameters also deviate from the expected temperature dependence at
110K, where the oxygen atoms in the vanadium oxide plane exhibit an increase in
positional disorder. The overall positional disorder of the apical oxygen of the
magnetic V+4 ion is also greater at all temperatures than the other oxygen
atoms. Weak supercell reflections appear in the powder diffraction patterns
below 40K. Bond length changes as a function of temperature indicate that the
V+4O5 ion rotates as the oxygen coordination polyhedra of the K atom collapses.
These and other structural changes are being used to construct a model for the
low temperature structure, and relate it to the changes in the transport and
dynamical properties.
[1] M.D. Lumsden et al., Phys. Rev. Lett. 86, 159-162
(2001).
[2] B.C. Sales et al., Phys. Rev. Lett. 88, 095901-4
(2002).
[3] J. Choi et al., Phys. Rev. B 65, 054101-6
(2001).
*Supported by the Division of Materials Sciences, U.S. D.O.E.
(contract DE-AC05-00OR22725 with UT-Battelle, LLC).