Abstract
Continued reduction in length scales associated with many ferroelectric film-based technologies is contingent on retaining the functional properties as the film thickness is reduced. Epitaxial and polycrystalline lead magnesium niobate-lead titanate (70PMN-30PT) thin films were studied over the thickness range of 100-350 nm for the relative contributions to property thickness dependence from interfacial and grain-boundary low permittivity layers. Epitaxial PMN-PT films were grown on SrRuO3/(001)SrTiO3, while polycrystalline films with {001}-Lotgering factors >0.96 were grown on Pt/TiO2/SiO2/Si substrates via chemical solution deposition. Both film types exhibited similar relative permittivities of ~300 at high fields at all measured thicknesses with highly crystalline electrode/dielectric interfaces. These results, with the DC-biased and temperature-dependent dielectric characterization, suggest irreversible domain wall mobility is the major contributor to the overall dielectric response and its thickness dependence. In epitaxial films, the irreversible Rayleigh coefficients reduced 85% upon decreasing thickness from 350 to 100 nm. The temperature at which a peak in the relative permittivity is observed was the only measured small signal quantity which was more thickness-dependent in polycrystalline than epitaxial films. This is attributed to the relaxor nature present in the films, potentially stabilized by defect concentrations, and/or chemical inhomogeneity. Finally, the effective interfacial layers are found to contribute to the measured thickness dependence in the longitudinal piezoelectric coefficient.
Original language | English |
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Pages (from-to) | 3961-3972 |
Number of pages | 12 |
Journal | Journal of the American Ceramic Society |
Volume | 100 |
Issue number | 9 |
DOIs | |
State | Published - Sep 2017 |
Externally published | Yes |
Funding
The authors gratefully acknowledge the transmission electron microscopy performed by Ke Wang at the Materials Characterization Laboratory of Penn State University and the technical assistance of Rick Spence, and Yang Ren at beamline 11-ID-C of the Advanced Photon Source at Argonne National Laboratory. This work was funded by the Penn State MRSEC, Center for Nanoscale Science, under the award NSF DMR-1420620, and by NSF DMR-1410907. JLJ and GE acknowledge support from the National Science Foundation under award number DMR-1409399. This publication was supported by the Pennsylvania State University Materials Research Institute Nanofabrication Laboratory. Use of the Advanced Photon Source, an Office of Science User Facility operated for the U.S. Department of Energy (DOE) Office of Science by Argonne National Laboratory, was supported by the U.S. DOE under Contract No. DE-AC02-06CH11357.
Funders | Funder number |
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Penn State MRSEC | |
U.S. DOE | DE-AC02-06CH11357 |
National Science Foundation | DMR-1409399, 1410907, 1409399 |
U.S. Department of Energy | |
Office of Science | |
Argonne National Laboratory | |
Center for Nanoscale Science and Technology | NSF DMR-1420620, DMR-1410907 |
Pennsylvania State University |
Keywords
- dielectric materials/properties
- ferroelectricity/ferroelectric materials
- piezoelectric materials/properties
- thin films