Pressure-induced phase-transition sequence in CoF2: An experimental and first-principles study on the crystal, vibrational, and electronic properties

J. A. Barreda-Argüeso, S. López-Moreno, M. N. Sanz-Ortiz, F. Aguado, R. Valiente, J. González, F. Rodríguez, A. H. Romero, A. Muñoz, L. Nataf, and F. Baudelet
Phys. Rev. B 88, 214108 – Published 19 December 2013

Abstract

We report a complete structural study of CoF2 under pressure. Its crystal structure and vibrational and electronic properties have been studied both theoretically and experimentally using first-principles density functional theory (DFT) methods, x-ray diffraction, x-ray absorption at Co K-edge experiments, Raman spectroscopy, and optical absorption in the 0–80 GPa range. We have determined the structural phase-transition sequence in CoF2 and corresponding transition pressures. The results are similar to other transition-metal difluorides such as FeF2 but different to ZnF2 and MgF2, despite that the Co2+ size (ionic radius) is similar to Zn2+ and Mg2+. We found that the complete phase-transition sequence is tetragonal rutile (P42/mnm) CaCl2 type (orthorhombic Pnnm) distorted PdF2 (orthorhombic Pbca)+PdF2 (cubic Pa3¯) in coexistence fluorite (cubic Fm3¯m) cotunnite (orthorhombic Pnma). It was observed that the structural phase transition to the fluorite at 15 GPa involves a drastic change of coordination from sixfold octahedral to eightfold cubic with important modifications in the vibrational and electronic properties. We show that the stabilization of this high-pressure cubic phase is possible under nonhydrostatic conditions since ideal hydrostaticity would stabilize the distorted-fluorite structure (tetragonal I4/mmm) instead. Although the first rutile CaCl2-type second-order phase transition is subtle by Raman spectroscopy, it was possible to define it through the broadening of the Eg Raman mode which is split in the CaCl2-type phase. First-principles DFT calculations are in fair agreement with the experimental Raman mode frequencies, thus providing an accurate description for all vibrational modes and elastic properties of CoF2 as a function of pressure.

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  • Received 16 September 2013

DOI:https://doi.org/10.1103/PhysRevB.88.214108

©2013 American Physical Society

Authors & Affiliations

J. A. Barreda-Argüeso1, S. López-Moreno2,*, M. N. Sanz-Ortiz1, F. Aguado1, R. Valiente3, J. González1, F. Rodríguez1, A. H. Romero4, A. Muñoz5, L. Nataf6, and F. Baudelet6

  • 1DCITIMAC, MALTA CONSOLIDER Team, Universidad de Cantabria, 39005 Santander, Spain
  • 2Escuela Superior Cd. Sahagún Universidad Autónoma del Estado de Hidalgo, Carretera Cd. Sahagún-Otumba s/n. 43990, Hidalgo, México
  • 3Departamento de Física Aplicada, MALTA CONSOLIDER Team, Universidad de Cantabria, 39005 Santander, Spain
  • 4Physics Department, West Virginia University, Morgantown, West Virginia, 26506-6315, USA
  • 5Departamento de Física Fundamental II, Instituto de Materiales y Nanotecnología Universidad de La Laguna, La Laguna 38205, Tenerife, Spain
  • 6Synchrotron SOLEIL, L'Orme des Merisiers, St Aubin BP48, 91192 Gif-sur-Yvette cedex, France

  • *Corresponding author: lsinhue@yahoo.com.mx

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Issue

Vol. 88, Iss. 21 — 1 December 2013

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