Experimental and theoretical study of α–Eu2(MoO4)3 under compression

The compression process in the α-phase of europium trimolybdate was revised employing several experimental techniques. X-ray diffraction (using synchrotron and laboratory radiation sources), Raman scattering and photoluminescence experiments were performed up to a maximum pressure of 21 GPa. In addi...

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Detalles Bibliográficos
Autores: Guzmán-Afonso, C., León-Luis, S.F., Sans-Tresserras, Juan Ángel, González -Silgo, C., Rodríguez-Hernández, Plácida, Radescu, S.,  Muñoz, A., López-Solano, J., Errandonea, D., Manjón, F.J., Rodríguez-Mendoza, U.R., Lavín, V.
Tipo de recurso: artículo
Fecha de publicación:2015
País:España
Institución:Universitat Politècnica de València (UPV)
Repositorio:RiuNet. Repositorio Institucional de la Universitat Politécnica de Valéncia
Idioma:inglés
OAI Identifier:oai:riunet.upv.es:10251/84613
Acceso en línea:https://riunet.upv.es/handle/10251/84613
Access Level:acceso abierto
Palabra clave:High pressure
X-ray diffraction
Raman scaterring
Photoluminescence
Rare earth trimolybdates
α-phase
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Descripción
Sumario:The compression process in the α-phase of europium trimolybdate was revised employing several experimental techniques. X-ray diffraction (using synchrotron and laboratory radiation sources), Raman scattering and photoluminescence experiments were performed up to a maximum pressure of 21 GPa. In addition, the crystal structure and Raman mode frequencies have been studied by means of first-principles density functional based methods. Results suggest that the compression process of α-Eu2(MoO4)3 can be described by three stages. Below 8 GPa, the α-phase suffers an isotropic contraction of the crystal structure. Between 8 and 12 GPa, the compound undergoes an anisotropic compression due to distortion and rotation of the MoO4 tetrahedra. At pressures above 12 GPa, the amorphization process starts without any previous occurrence of a crystalline-crystalline phase transition in the whole range of pressure. This behavior clearly differs from the process of compression and amorphization in trimolybdates with β′-phase and tritungstates with α-phase.