Crystallographic Structure and Ferroelectricity of (AxLa1−x)2Ti2O7 (A = Sm and Eu) Solid Solutions with High Tc
The solubility and ferroelectric properties of (AxLa1−x)2Ti2O7 (A = Sm and Eu) solid solutions were investigated. The crystallographic structure of the solid solutions was studied using X‐ray diffraction and Raman spectroscopy. The solubility limits of Eu and Sm in (AxLa1−x) 2Ti2O7 were found to be...
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Published in | Journal of the American Ceramic Society Vol. 99; no. 2; pp. 523 - 530 |
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Main Authors | , , , |
Format | Journal Article |
Language | English |
Published |
Columbus
Blackwell Publishing Ltd
01.02.2016
Wiley Subscription Services, Inc |
Subjects | |
Online Access | Get full text |
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Summary: | The solubility and ferroelectric properties of (AxLa1−x)2Ti2O7 (A = Sm and Eu) solid solutions were investigated. The crystallographic structure of the solid solutions was studied using X‐ray diffraction and Raman spectroscopy. The solubility limits of Eu and Sm in (AxLa1−x) 2Ti2O7 were found to be greater than x = 0.5 and 0.8, respectively. The solid solutions had a monoclinic perovskite‐like layered structure (PLS), similar to that of the pure La2Ti2O7, when x was less than the solubility limit. When x was above the solubility limit the materials were biphase. The biphases of (SmxLa1−x)Ti2O7 (x = 0.9) consisted of (SmxLa1−x)2Ti2O7 with PLS and pure Sm2Ti2O7 with pyrochlore structure, and the biphases of (EuxLa1−x)Ti2O7 (x = 0.6, 0.7, and 0.8) consisted of (EuxLa1−x)2Ti2O7 with PLS structure and La3+ doped Eu2Ti2O7 with pyrochlore structure. The effect of A‐site substitution on the properties of La2Ti2O7 was investigated by measuring the dielectric permittivity and loss at different frequencies and temperatures. The highest piezoelectric constant d33 was 2.8 pC/N for (Sm0.1La0.9)Ti2O7. |
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Bibliography: | Meggitt Sensing Systems ark:/67375/WNG-PL9D0QHQ-F ArticleID:JACE13970 istex:FEEEE90C4078FABCCCB26C7DA26A8ECCAF33EA66 China Scholarship Council (CSC) |
ISSN: | 0002-7820 1551-2916 |
DOI: | 10.1111/jace.13970 |