Published September 2009 | Version v1
Journal article

The magnetic structure of clinopyroxene-type LiFeGe2O6 and revised data on multiferroic LiFeSi2O6

  • 1. Department of Materials Engineering and Physics, Division of Mineralogy, University of Salzburg, Hellbrunnertstr. 34, A-5020 Salzburg (Austria)
  • 2. Institute of Crystallography, RWTH Aachen University, Jaegerstr. 17/19, D-52056 Aachen (Germany)
  • 3. Institute of Mineralogy, Philipps-University Marburg, Hans Meerweinstr., D-35032 Marburg/Lahn (Germany)
  • 4. Institute for Materials Science, Darmstadt University of Technology, Petersenstrasse 23, 64287 Darmstadt c/o FRM II, Lichtenbergstrasse 1, 85747 Garching (Germany)
  • 5. Sciences Chimiques de Rennes - UMR 6226, Materiaux Inorganiques: Chimie Douce et Reactivite, Universite de Rennes 1, Campus de Beaulieu, Bat 10B, F-35042 Rennes (France)
  • 6. Laboratoire Leon Brillouin (UMR12 CEA-CNRS), CEA-Saclay, F-91191 Gif-Sur-Yvette Cedex (France)
  • 7. Department of Chemistry, Philipps-University Marburg, Hans Meerweinstr., D-35032 Marburg/Lahn (Germany)

Description

The clinopyroxene compounds LiFeSi2O6 and LiFeGe2O6 have been investigated by constant wavelength neutron diffraction at low temperatures and by bulk magnetic measurements. Both compounds are monoclinic, space group P21/c and do not exhibit a change in nuclear symmetry down to 1.4 and 5 K respective. However, they transform to a magnetically ordered state below 20 K. LiFeSi2O6 shows a simple magnetic structure with no indication of an incommensurate modulation. The magnetic space group is P21/c' and the structure is described by a ferromagnetic coupling of spins within the infinite M1 chains of edge-sharing octahedra, while the coupling between these M1 chains is antiferromagnetic. The magnetic phase transition is accompanied by magnetostriction of the lattice when passing through the magnetic phase transition. The magnetic structure of LiFeGe2O6 is different to the silicate: the space group is P21'/c and the magnetic unit cell doubled along the a-direction. Within the M1 chains spins are coupled antiferromagnetically, while the chain to chain coupling is antiferromagnetic when coupling goes via the GeB tetrahedron and ferromagnetic when it goes via the GeA tetrahedron. - Graphical abstract: Section of the nuclear and magnetic structure of the synthetic clinopyroxene-type compound LiFeGe2O6 displaying the antiferromagnetic coupling of spins within the chains of Fe3+O6 octahedra and the antiferromagnetic (via GeB sites) and ferromagnetic (via GeA sites) coupling between these chains.

Availability note (English)

Available from http://dx.doi.org/10.1016/j.jssc.2009.06.013

Additional details

Identifiers

DOI
10.1016/j.jssc.2009.06.013;
PII
S0022-4596(09)00259-X;

Publishing Information

Journal Title
Journal of Solid State Chemistry
Journal Volume
182
Journal Issue
9
Journal Page Range
p. 2374-2384
ISSN
0022-4596
CODEN
JSSCBI

Optional Information

Copyright
Copyright (c) 2009 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.