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Fizika Tverdogo Tela, 2015 Volume 57, Issue 3, Pages 475–479 (Mi ftt11375)

This article is cited in 9 papers

Proceedings of the XX All-Russia Conference on Physics of Ferroelectrics (VKS-XX)

Phase transitions in two- and three-component perovskite superlattices

Yu. A. Tikhonova, A. G. Razumnayaab, O. A. Maslovaa, I. N. Zakharchenkoa, Yu. I. Yuzyuka, N. Ortegac, A. Kumarc, R. S. Katiyarc

a Southern Federal University, Rostov-on-Don
b LPMC, Université de Picardie Jules Verne, Amiens, France
c University of Puerto Rico, San Juan, Puerto Rico, USA

Abstract: The temperature behavior of polarization Raman spectra of two-layer BaTiO$_3$/Ba$_{0.5}$Sr$_{0.5}$TiO$_3$/SrTiO$_3$ and three-layer BaTiO$_3$/Ba$_{0.5}$Sr$_{0.5}$TiO$_3$/SrTiO$_3$ superlattices prepared by pulsed laser deposition on (001)MgO substrates has been studied. It has been found that, at room temperature, the frequency of soft mode $E$(TO) in the three-layer superlattice is significantly higher (94 cm$^{-1}$) than that in the two-layer superlattice (70 cm$^{-1}$), which demonstrates an increase in two-dimensional stresses in epitaxial layers of the superlattice. An analysis of the temperature dependence of the integrated intensity of soft mode $E$(TO) suggests that the BaTiO$_3$/Ba$_{0.5}$Sr$_{0.5}$TiO$_3$/SrTiO$_3$ superlattice undergoes a transition from the ferroelectric to paraelectric phase at $\sim$ 540 K, and the phase transition temperature of the BaTiO$_3$/Ba$_{0.5}$Sr$_{0.5}$TiO$_3$/SrTiO$_3$ superlattice increases to $\sim$ 610 K because of the deformation of the epitaxial layers.


 English version:
Physics of the Solid State, 2015, 57:3, 486–490

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