Research master thesis: Why is calcium titanate antiferrodistortive, while lead zirconate is antiferroelectric?
Chao, Chih-Hsuan
Promotor(s) : Ghosez, Philippe
Date of defense : 6-Sep-2022/7-Sep-2022 • Permalink : http://hdl.handle.net/2268.2/16133
Details
Title : | Research master thesis: Why is calcium titanate antiferrodistortive, while lead zirconate is antiferroelectric? |
Author : | Chao, Chih-Hsuan |
Date of defense : | 6-Sep-2022/7-Sep-2022 |
Advisor(s) : | Ghosez, Philippe |
Committee's member(s) : | Dorbolo, Stéphane
Nguyen, Ngoc Duy Schlagheck, Peter |
Language : | English |
Discipline(s) : | Physical, chemical, mathematical & earth Sciences > Physics |
Institution(s) : | Université de Liège, Liège, Belgique |
Degree: | Master en sciences physiques, à finalité approfondie |
Faculty: | Master thesis of the Faculté des Sciences |
Abstract
[en] Antiferroelectric (AFE) materials have been of interest in the application of high-energy-density
capacitors and strain-induced actuators. However, there are only a few identified AFE materials,
most belong to oxide perovskites, such as PbZrO3, PbHfO3, and NaNbO3. We rationalize the
limited number by providing their restricted criteria. The ground state of an AFE is nonpolar
and experiences a phase transition to a symmetry-related polar phase under a sufficiently large
electric field. To exhibit the phase transition, the energy of the polar phase should be close to the
nonpolar ground state and their energy barrier should be flat enough. For the nonpolar perovskites,
it is commonplace that the high energy barrier hinders the AFE characteristic. The purpose of
the thesis is to understand the microscopic origin of the flat energy barrier in the prototypical
AFE material, PbZrO3. We make this by comparing PbZrO3 to CaTiO3 in the second-principles
models since these two materials share similar structures at high temperatures. We identify that
the difference in atomic interactions, Pb-O in PbZrO3 and Ca-O in CaTiO3, is crucial for the
energy barrier between the nonpolar ground states and the polar phases. Additionally, by tuning
the coefficients, we reproduce the nonpolar-polar phase transition path of PbZrO3 on the CaTiO3
second-principles model. The Pb-O interactions cannot be reproduced by the hydrostatic pressure in CaTiO3.
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