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Relation between Fractal Inhomogeneity and In/Nb-Arrangement in Pb(In(1/2)Nb(1/2))O(3)

Relaxor ferroelectrics show substantial responses to electric fields. The key difference from normal ferroelectrics is a temperature-dependent inhomogeneous structure and its dynamics. The lead-based complex perovskite Pb(In(1/2)Nb(1/2))O(3) is an intriguing system in which the inhomogeneous structu...

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Detalles Bibliográficos
Autores principales: Tsukada, Shinya, Ohwada, Kenji, Ohwa, Hidehiro, Mori, Shigeo, Kojima, Seiji, Yasuda, Naohiko, Terauchi, Hikaru, Akishige, Yukikuni
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5727483/
https://www.ncbi.nlm.nih.gov/pubmed/29235499
http://dx.doi.org/10.1038/s41598-017-17349-3
Descripción
Sumario:Relaxor ferroelectrics show substantial responses to electric fields. The key difference from normal ferroelectrics is a temperature-dependent inhomogeneous structure and its dynamics. The lead-based complex perovskite Pb(In(1/2)Nb(1/2))O(3) is an intriguing system in which the inhomogeneous structure can be controlled by thermal treatment. Herein, we report investigations of the phase transitions in single crystals of Pb(In(1/2)Nb(1/2))O(3) via changing the degree of randomness in which In and Nb occupy the B site of the ABO(3) perovskite structure. We studied the dynamic properties of the structure using inelastic light scattering and the static properties using diffuse X-ray scattering. These properties depend on the degree of randomness with which the B site is occupied. When the distribution of occupied In/Nb sites is regular, the antiferroelectric phase is stabilised by a change in the collective transverse-acoustic wave, which suppresses long-range ferroelectric order and the growth of the inhomogeneous structure. However, when the B site is occupied randomly, a fractal structure grows as the temperature decreases below T (*)~475 K, and nanosized ferroelectric domains are produced by the percolation of self-similar and static polar nanoregions.