2012
DOI: 10.1021/cm303059h
|View full text |Cite
|
Sign up to set email alerts
|

La-Driven Morphotrophic Phase Boundary in the Bi(Zn1/2Ti1/2)O3–La(Zn1/2Ti1/2)O3–PbTiO3 Solid Solution

Abstract: We explore the Bi(Zn1/2Ti1/2)O3–La(Zn1/2Ti1/2)O3–PbTiO3 pseudoternary phase diagram using density functional theory and a solid solution model. We find a region of stability against phase segregation that contains a morphotropic phase boundary. On the basis of the results, we identify a ferroelectrically active composition-dependent region that is likely to show strong electro-mechanical response. Furthermore, we find that La replacement for Bi not only lowers the polarization as might be expected, but also sh… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4

Citation Types

0
7
0

Year Published

2014
2014
2023
2023

Publication Types

Select...
9

Relationship

1
8

Authors

Journals

citations
Cited by 14 publications
(7 citation statements)
references
References 36 publications
0
7
0
Order By: Relevance
“…PbTiO 3 -type bismuth-based perovskites, including BiCoO 3 ( c / a = 1.27; P S = 126 μC/cm 2 by the point charge model), , Bi 2 ZnTiO 6 ( c / a = 1.21; P S = 103 μC/cm 2 by the point charge model), and Bi 2 ZnVO 6 ( c / a = 1.26; P S = 126 μC/cm 2 by the point charge model), have recently been found. The giant spontaneous polarization inhibits the polarization reversal and appearance of a large piezoelectric response. , Chemical substitution attempts in Bi 2 ZnTiO 6 , such as La 3+ for Bi 3+ , Mg 2+ for Zn 2+ , and Mn 4+ for Ti 4+ , have been made to reduce the level of spontaneous polarization. However, the magnitudes of spontaneous polarization hardly decreased in the tetragonal phases of Bi 2– x La x ZnTiO 6 ( x < 0.3) and Bi 2 Zn 1– x Mg x TiO 6 ( x < 0.3). The crystal structure changed to the monoclinic Ia ( Cc ) phase in Bi 2 ZnTi 1– x Mn x O 6 (0.2 ≤ x ≤ 0.45).…”
Section: Introductionmentioning
confidence: 99%
“…PbTiO 3 -type bismuth-based perovskites, including BiCoO 3 ( c / a = 1.27; P S = 126 μC/cm 2 by the point charge model), , Bi 2 ZnTiO 6 ( c / a = 1.21; P S = 103 μC/cm 2 by the point charge model), and Bi 2 ZnVO 6 ( c / a = 1.26; P S = 126 μC/cm 2 by the point charge model), have recently been found. The giant spontaneous polarization inhibits the polarization reversal and appearance of a large piezoelectric response. , Chemical substitution attempts in Bi 2 ZnTiO 6 , such as La 3+ for Bi 3+ , Mg 2+ for Zn 2+ , and Mn 4+ for Ti 4+ , have been made to reduce the level of spontaneous polarization. However, the magnitudes of spontaneous polarization hardly decreased in the tetragonal phases of Bi 2– x La x ZnTiO 6 ( x < 0.3) and Bi 2 Zn 1– x Mg x TiO 6 ( x < 0.3). The crystal structure changed to the monoclinic Ia ( Cc ) phase in Bi 2 ZnTi 1– x Mn x O 6 (0.2 ≤ x ≤ 0.45).…”
Section: Introductionmentioning
confidence: 99%
“…Such random alloys represent a major challenge for first-principles calculations due to the limited size of the computational supercells that can be simulated. Typically, the structure and properties of an alloy are studied using small supercells, approximating the alloy compositions with highly ordered structures [5][6][7]. For compounds with simple ratios, like KNN, a rocksalt structure (RSS) is often used [8].…”
Section: Introductionmentioning
confidence: 99%
“…1,2 PbTiO 3 -based perovskite compounds are significant multifunction materials, which have been extensively researched in the last half century. [3][4][5] Through chemical modification, we can manipulate the physical properties of these compounds like ferroelectric, piezoelectric, and other properties. 6 Recently, Bi-based perovskites of BiMeO 3 , in which Me are cations with an average valent of þ3, have been adopted to form a binary system with PbTiO 3 , so that the high temperature ferroelectric properties are optimized.…”
mentioning
confidence: 99%