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Phys. Rev. B 79, 104115 (2009) [6 pages]

Phonons in the cubic phase of Co3B7O13X (X=Cl, Br, and I) boracites

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J. Pascual
Institut Català de Nanotecnologia (ICN) Edifici CM7, Campus de la UAB, 08193 Bellaterra, Barcelona, Spain and Departament de Física Edifici Cn, Universitat Autònoma de Barcelona, 08193 Bellaterra, Barcelona, Spain

Jorge Íñiguez
Institut de Ciencia de Materials de Barcelona (ICMAB-CSIC), Campus UAB, 08193 Bellaterra, Spain

M. N. Iliev, V. G. Hadjiev, and J. Meen
Texas Center for Superconductivity, University of Houston, Texas 77204-5002, USA

Received 8 December 2008; revised 4 February 2009; published 30 March 2009

The phonon structure in the cubic paraelectric phase (F4̅ 3c) of Co3B7O13X (X=Cl,Br,I) boracites has been studied theoretically by density-functional theory and experimentally by Raman spectroscopy. The calculated Raman frequencies are in good agreement with those determined from the polarized Raman spectra. In addition to the four Raman-allowed phonons of A1 symmetry, a low-frequency broadband of same symmetry is observed in the spectra of Co3B7O13Cl and Co3B7O13Br. The position and width of this band correspond to those of the partial phonon density of states of the halogen vibrations: an indication for disorder and instability of the halogen sublattice. In the case of Co3B7O13I, an even greater number of spectral features reflecting the underlying phonon density of states are observed. An “instability” F2 mode that involves displacements of the X atoms along ⟨111⟩ and of the Co atoms along ⟨100⟩ directions is also identified. It is shown that this mode is closely related to the halogen and metal sublattice instabilities, which trigger the cubic to orthorhombic transition at lower temperature.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.79.104115
DOI:
10.1103/PhysRevB.79.104115
PACS:
78.30.−j, 77.84.Bw, 78.20.Bh, 79.60.Ht