Domain patterns in epitaxial rhombohedral ferroelectric films. I. Geometry and experiments

被引:272
|
作者
Streiffer, SK
Parker, CB
Romanov, AE
Lefevre, MJ
Zhao, L
Speck, JS
Pompe, W
Foster, CM
Bai, GR
机构
[1] N Carolina State Univ, Dept Mat Sci & Engn, Raleigh, NC 27695 USA
[2] Max Planck Inst Met Forsch, D-70174 Stuttgart, Germany
[3] Univ Calif Santa Barbara, Dept Mat, Santa Barbara, CA 93106 USA
[4] Tech Univ Dresden, D-01069 Dresden, Germany
[5] Argonne Natl Lab, Div Mat Sci, Argonne, IL 60439 USA
[6] Russian Acad Sci, AF Ioffe Physicotech Inst, St Petersburg 194021, Russia
关键词
D O I
10.1063/1.366632
中图分类号
O59 [应用物理学];
学科分类号
摘要
Possible domain patterns are developed for (001) oriented (pseudocubic indexing) epitaxial rhombohedral perovskite ferroelectric (F-R) films. We assume that the films are grown above their Curie temperature (T-C) in a cubic paraelectric (P-C) state, The rhombohedral distortion consists of a "stretch" along one of the four [111] crystallographic directions of the cubic perovskite unit cell. Domain pattern formation is concurrent with the P-C-->F-R transformation on cooling from the growth temperature. The domain patterns form to minimize elastic energy in the film, at the energetic expense of both forming domain boundaries and developing local stresses in the substrate. Eight possible domains may form, half of which are related by inversion, thus leading to four mechanically distinct variants. The possible domain walls are determined by mechanical and charge compatibility and follow closely from the analysis of Fousek and Janovec [J. Appl. Phys. 40, 135 (1969)]. Domain patterns may develop with either {100} or {101} boundaries. In both cases, the individual domains in the patterns are energetically degenerate and thus equal width lamellar patterns are predicted. When polarization is included in the analysis, the {100} boundary patterns have no normal component of the net polarization, whereas the {101} boundary patterns correspond to the fully poled state. We report on experimental observation of {100} domain patterns in epitaxial PbZr0.80Ti0.20O3 and PbZr0.65Ti0.35O3 films. (C) 1998 American Institute of Physics.
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页码:2742 / 2753
页数:12
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