Hostname: page-component-78c5997874-lj6df Total loading time: 0 Render date: 2024-11-13T14:33:26.418Z Has data issue: false hasContentIssue false

Antiferroelectric to Paraelectric Phase Transition in Lead Zirconate Thin Films

Published online by Cambridge University Press:  10 February 2011

D.M. Fanning
Affiliation:
Dept. of Physics Dept. of Materials Science and Engineering, University of Illinois, Urbana, IL 61801td-fanni@uiuc.edu
I.K. Robinson
Affiliation:
Dept. of Physics Dept. of Materials Science and Engineering, University of Illinois, Urbana, IL 61801
T. Tani
Affiliation:
Dept. of Physics Dept. of Materials Science and Engineering, University of Illinois, Urbana, IL 61801
D. A. Payne
Affiliation:
Dept. of Physics Dept. of Materials Science and Engineering, University of Illinois, Urbana, IL 61801
Get access

Abstract

Lead zirconate, PbZrO3, is antiferroelectric at room temperature and has a first-order phase transition to the paraelectric state at 230°C in bulk crystals. At room temperature, the antiferroelectric Pb displacements along [110] directions produce a superstructure at the (h+¼ k+¼, 1) positions (referenced to pseudo-tetragonal unit cell). The Pb displacements occur perpendicular to the shorter c axis. In this study, the behavior of thin films was compared to the bulk. Films of lead zirconate were deposited onto electroded silicon wafers via the sol gel method. By varying the deposition conditions of the Pt substrate, films with both {111} and {100} preferred orientation were grown. The crystalline film consisted of columnar grains which were not completely aligned with each other, but had a random orientation with respect to the film's perpendicular axis. Measurements of superstructure peak intensities vs. temperature show that the thin films exhibit a much more gradual phase transition to the paraelectric state compared to the bulk. Furthermore, comparison of a and c vs. temperature show this effect, as well as a strain of about 0.5% in c. In the {100} oriented films, we found that the c-axis was oriented perpendicular to the film's surface, meaning they should be classified as (001).

Type
Research Article
Copyright
Copyright © Materials Research Society 1999

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

1. Sawaguchi, E., J. of Phys. Soc. of Japan, 8 [5], p. 615, 1953.Google Scholar
2. Tani, T., Li, J., Viehland, D., Payne, D., J. Appl. Phys. 75 (6), p. 3017, 1994.Google Scholar
3. Fujishita, H., Hoshino, S., J. of Phys. Soc. of Japan, 53 [1], p. 226, 1984.Google Scholar