*Member, The American Ceramic Society.
Origins of Electro-Mechanical Coupling in Polycrystalline Ferroelectrics During Subcoercive Electrical Loading
Article first published online: 18 JAN 2011
© 2011 The American Ceramic Society
Journal of the American Ceramic Society
Volume 94, Issue 2, pages 293–309, February 2011
How to Cite
Pramanick, A., Damjanovic, D., Daniels, J. E., Nino, J. C. and Jones, J. L. (2011), Origins of Electro-Mechanical Coupling in Polycrystalline Ferroelectrics During Subcoercive Electrical Loading. Journal of the American Ceramic Society, 94: 293–309. doi: 10.1111/j.1551-2916.2010.04240.x
D. J. Green—contributing editor
This work was supported by the U.S. National Science Foundation (NSF) under award numbers DMR-0746902 and OISE-0755170, and the U.S. Department of the Army under W911NF-09-1-0435.
- Issue published online: 7 FEB 2011
- Article first published online: 18 JAN 2011
- Manuscript No. 28530. Received August 31, 2010; approved October 5, 2010.
The electromechanical coupling in ferroelectric materials is controlled by several coexisting structural phenomena which can include piezoelectric lattice strain, 180° and non-180° domain wall motion, and interphase boundary motion. The structural mechanisms that contribute to electromechanical coupling have not been readily measured in the past, particularly under the low-to-medium driving electric field amplitudes at which many piezoelectric materials are used. In this feature, results from in situ, high-energy, and time-resolved X-ray diffraction experiments are interpreted together with macroscopic piezoelectric coefficient measurements in order to better understand the contribution of these mechanisms to the electromechanical coupling of polycrystalline ferroelectric materials. The compositions investigated include 2 mol% La-doped PbZr0.60Ti0.40O3, 2 mol% La-doped PbZr0.52Ti0.48O3, 2 mol% La-doped PbZr0.40Ti0.60O3, undoped PbZr0.52Ti0.48O3, and 2 mol% Fe-doped PbZr0.47Ti0.53O3. In all compositions, a strong correlation is found between the field-amplitude-dependence of the macroscopic piezoelectric coefficient and the contribution of non-180° domain wall motion determined from the diffraction data. The results show directly that the Rayleigh-like behavior of d33 piezoelectric coefficient is predominantly due to a Rayleigh-like behavior of non-180° domain wall motion. Furthermore, after separating contributions from lattice (atomic level) and domain wall motion (nanoscale level) to the measured macroscopic piezoelectric properties, we show that previously ignored intergranular interactions (microscopic level) account for a surprisingly large portion of the electromechanical coupling. These results demonstrate that electromechanical coupling in polycrystalline aggregates is substantially different from that observed in single crystalline materials. The construct of emergence is used to describe how averaged macrolevel phenomena are different from the material response observed in an isolated subcomponent of the material. Consequently, and due to its size-scale complexity, the description of grain-to-grain interactions is presently inaccessible in most ab initio and phenomenological approaches. Results presented here demonstrate the need to account for these interactions in order to completely describe macroscopic electromechanical properties of polycrystalline materials.