Abstract
The piezoelectric material (1-x)Ba(Zr 0.2 Ti 0.8 )O 3 -x(Ba 0.7 Ca 0.3 )TiO 3 (BZT-xBCT) has emerged as a leading lead-free candidate to replace Pb(Zr 1-x Ti x )O 3 (PZT) for certain applications. However, the structural response of BZT-xBCT to an electric field is not well understood, particularly how the local structure responds to varying electric fields. In this study, in situ synchrotron X-ray diffraction and total scattering measurements were performed on BZT-xBCT from x = 0.45 to 0.60. The lattice distortions were quantified from the unit cell parameters for the compositions in the orthorhombic (O) region (x = 0.45 to 0.50) and tetragonal (T) region (x = 0.51 to 0.60). It was found that the lattice distortion is minimized in compositions that exhibit the largest effective piezoelectric effect, particularly at the x = 0.45 composition (between the rhombohedral (R) and O regions) and at the morphotropic phase boundary (MPB) composition x = 0.50 (between O and T regions). The degree of domain wall motion was quantified, and the results indicate that as the MPB is approached, the degree of domain wall motion increases dramatically. The increase in domain wall motion also coincides with the minimization of the lattice distortion. The pair distribution functions (PDFs) were calculated from the Fourier transform of the total scattering data. Analysis of the PDF peak shifts with electric field shows nonlinear lattice strains across all compositions, which indicates a deviation from classical piezoelectric behavior. We conclude that the strong piezoelectric properties in the BZT-xBCT system are attributed to an increased degree of domain wall reorientation that is facilitated by a decreased lattice distortion.
Original language | English |
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Pages (from-to) | 79-91 |
Number of pages | 13 |
Journal | Acta Materialia |
Volume | 171 |
DOIs | |
State | Published - Jun 1 2019 |
Externally published | Yes |
Funding
Michelle Dolgos, Alicia Manjón-Sanz, and Charles Culbertson would like to thank the National Science Foundation (NSF) under Grant No. DMR-1606909. This research used resources of the Advanced Photon Sciences, a U.S. Department of Energy Office of Science User Facility operated for the DOE Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357. Jacob Jones acknowledges support from the NSF under award number DMR-1409399. We would like to thank Kevin Beyer, Olaf Borkiewicz, and Changhao Zhao for their assistance with running the experiment on 11-ID-B at the Advanced Photon Source. In addition, we would also like to thank Anton Goetzee-Barral for insightful conversations about the PDF analysis. Michelle Dolgos, Alicia Manjón-Sanz, and Charles Culbertson would like to thank the National Science Foundation (NSF) under Grant No. DMR-1606909 . This research used resources of the Advanced Photon Sciences, a U.S. Department of Energy Office of Science User Facility operated for the DOE Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357 . Jacob Jones acknowledges support from the NSF under award number DMR-1409399 . We would like to thank Kevin Beyer, Olaf Borkiewicz, and Changhao Zhao for their assistance with running the experiment on 11-ID-B at the Advanced Photon Source. In addition, we would also like to thank Anton Goetzee-Barral for insightful conversations about the PDF analysis.
Funders | Funder number |
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DOE Office of Science | |
U.S. Department of Energy Office of Science | |
National Science Foundation | DMR-1606909 |
National Sleep Foundation | |
Argonne National Laboratory | DMR-1409399 |
Keywords
- Ferroelectric
- Morphotropic phase boundary
- Piezoelectric
- X-ray diffraction