Producción Científica Profesorado

2012

López-Moreno, S., Romero, A. H., Mejía-López, J., Muñoz, A., & Roshchin, I. V. (2012). First-principles study of electronic, vibrational, elastic, and magnetic properties of FeF2 as a function of pressure. Physical Review B 85, 134110. doi: 10.1103/PhysRevB.85.134110

**Abstract**

We report systematic ab initio calculations of the electronic band structure, phonon dispersion relation, and the structural characterization of FeF2 in the rutile (P42/mnm) structure as well as in several high-pressure phases by means of the generalized gradient approximation (GGA)+U approximation. Using the phonon dispersion relations, we calculated the Gibbs free energy and evaluated the phase transitions at 300 K, at which most experimental measurements are performed. Calculated Raman and infrared vibrational modes, lattice parameters, and electronic structure for all considered crystalline structures are compared with available experimental data. Our calculations show that at 5.33 GPa, the FeF2 undergoes a second-order proper ferroelastic phase transition, rutile ? CaCl2-type structure. This result is supported by the softening of the elastic shear module Cs in the rutile phase, the softening (hardening) of the B1g (Ag) Raman active mode in the rutile (CaCl2-type) structure near the transition pressure, and the decrease of the square of the spontaneous strain ess from the CaCl2-type structure. This demonstrates that the rutile ? CaCl2-type phase transition is driven by the coupling between the Raman active B1g mode and shear modulus Cs. At 8.22 GPa, the CaCl2-type structure undergoes a first-order phase transition to the Pbca phase, a distorted fcc Pa3? phase with a volume reduction of ?V?7%, as reported in experiments. Upon further increase of the pressure, the Pbca phase transforms to a Fmmm phase othorhombic center-type structure at ?20.38 GPa, with ?V?2.5%. Finally, at 25.05 GPa, there is a phase transition to the orthorhombic cotunnite structure (Pnma space group), with ?V?5.8%, which is stable up to 45 GPa, the largest considered pressure. The coordination number for the Fe ion in each phase is 6, 6, 6, 8, and 9 for rutile, CaCl2-type, Pbca, Fmmm, and cotunnite structures, respectively. The evolution of the band gap, phonon frequencies, and magnetic moment of Fe ion as a function of the applied pressure is reported for all studied phases. The exchange constants J1, J2, and J3, calculated for rutile and the lowest Gibbs free-energy high-pressure phases, are reported.