Phase behaviour of Ag2CrO4 under compression: Structural, vibrational, and optical properties

We have performed an experimental study of the crystal structure, lattice dynamics, and optical properties of silver chromate (Ag2CrO4) at ambient temperature and high pressures. In particular, the crystal structure, Raman-active phonons, and electronic band gap have been accurately determined. When...

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Detalhes bibliográficos
Autores: Santamaría Pérez, David, Errandonea, Daniel, Ruiz-Fuertes, Javier, Sans, Juan Ángel, Rodríguez-Hernández, Plácida, Muñoz, Alfonso, Bandiello, Enrico|||0000-0003-0956-3195, Gomis, O.|||0000-0001-6763-0638, Manjón, Francisco-Javier|||0000-0002-3926-1705
Formato: artículo
Fecha de publicación:2013
País:España
Recursos:Universitat Politècnica de València (UPV)
Repositorio:RiuNet. Repositorio Institucional de la Universitat Politécnica de Valéncia
Idioma:inglés
OAI Identifier:oai:riunet.upv.es:10251/38674
Acesso em linha:https://riunet.upv.es/handle/10251/38674
Access Level:acceso abierto
Palavra-chave:X-Ray Diffraction
Total-Energy calculations
Augmented-wave method
Crystal-structure
Silver cromate
High-pressures
Potassium chromate
Transition
Raman
Antifluorite
FISICA APLICADA
Descrição
Resumo:We have performed an experimental study of the crystal structure, lattice dynamics, and optical properties of silver chromate (Ag2CrO4) at ambient temperature and high pressures. In particular, the crystal structure, Raman-active phonons, and electronic band gap have been accurately determined. When the initial orthorhombic Pnma Ag2CrO4 structure (phase I) is compressed up to 4.5 GPa, a previously undetected phase (phase II) has been observed with a 0.95% volume collapse. The structure of phase II can be indexed to a similar orthorhombic cell as phase I, and the transition can be considered to be an isostructural transition. This collapse is mainly due to the drastic contraction of the a axis (1.3%). A second phase transition to phase III occurs at 13 GPa to a structure not yet determined. First-principles calculations have been unable to reproduce the isostructural phase transition, but they propose the stabilization of a spinel-type structure at 11 GPa. This phase is not detected in experiments probably because of the presence of kinetic barriers. Experiments and calculations therefore seem to indicate that a new structural and electronic description is required to model the properties of silver chromate.