Low temperature dielectric relaxation in ordinary perovskite ferroelectrics: enlightenment from high-energy x-ray diffraction

Ordinary ferroelectrics exhibit a second order phase transition that is characterized by a sharp peak in the dielectric permittivity at a frequency-independent temperature. Furthermore, these materials show a low temperature dielectric relaxation that appears to be a common behavior of perovskite sy...

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Detalles Bibliográficos
Autores: Ochoa Guerrero, Diego A.|||0000-0002-8756-9704, Levit Valenzuela, Rafael, Fancher, Christopher M., Esteves, Giovanni, Jones, Jacob L., García García, José Eduardo|||0000-0002-1232-1739
Tipo de recurso: artículo
Fecha de publicación:2017
País:España
Institución:Universitat Politècnica de Catalunya (UPC)
Repositorio:UPCommons. Portal del coneixement obert de la UPC
Idioma:inglés
OAI Identifier:oai:upcommons.upc.edu:2117/103927
Acceso en línea:https://hdl.handle.net/2117/103927
https://dx.doi.org/10.1088/1361-6463/aa6b9e
Access Level:acceso abierto
Palabra clave:Ferroelectric crystals
Piezoelectric materials
Dielectric relaxation
ferroelectrics
piezoelectric materials
dielectric response
dielectric relaxation
Cristalls ferroelectrics
Materials piezoelèctrics
Relaxació dielèctrica
Àrees temàtiques de la UPC::Física
Descripción
Sumario:Ordinary ferroelectrics exhibit a second order phase transition that is characterized by a sharp peak in the dielectric permittivity at a frequency-independent temperature. Furthermore, these materials show a low temperature dielectric relaxation that appears to be a common behavior of perovskite systems. Tetragonal lead zirconate titanate is used here as a model system in order to explore the origin of such an anomaly, since there is no consensus about the physical phenomenon involved in it. Crystallographic and domain structure studies are performed from temperature dependent synchrotron x-ray diffraction measurement. Results indicate that the dielectric relaxation cannot be associated with crystallographic or domain configuration changes. The relaxation process is then parameterized by using the Vogel–Fulcher–Tammann phenomenological equation. Results allow us to hypothesize that the observed phenomenon is due to changes in the dynamic behavior of the ferroelectric domains related to the fluctuation of the local polarization.