Premium
New method to measure domain‐wall motion contribution to piezoelectricity: the case of PbZr 0.65 Ti 0.35 O 3 ferroelectric
Author(s) -
Gorfman Semën,
Choe Hyeokmin,
Zhang Guanjie,
Zhang Nan,
Yokota Hiroko,
Glazer Anthony Michael,
Xie Yujuan,
Dyadkin Vadim,
Chernyshov Dmitry,
Ye Zuo-Guang
Publication year - 2020
Publication title -
journal of applied crystallography
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.429
H-Index - 162
ISSN - 1600-5767
DOI - 10.1107/s1600576720008213
Subject(s) - electric field , diffraction , ferroelectricity , piezoelectricity , condensed matter physics , domain wall (magnetism) , physics , lattice (music) , lattice constant , materials science , optics , magnetic field , dielectric , magnetization , quantum mechanics , acoustics
A new data analysis routine is introduced to reconstruct the change in lattice parameters in individual ferroelastic domains and the role of domain‐wall motion in the piezoelectric effect. Using special electronics for the synchronization of a PILATUS X‐ray area detector with a voltage signal generator, the X‐ray diffraction intensity distribution was measured around seven split Bragg peaks as a function of external electric field. The new data analysis algorithm allows the calculation of `extrinsic' (related to domain‐wall motion) and `intrinsic' (related to the change in lattice parameters) contributions to the electric‐field‐induced deformation. Compared with previously existing approaches, the new method benefits from the availability of a three‐dimensional diffraction intensity distribution, which enables the separation of Bragg peaks diffracted from differently oriented domain sets. The new technique is applied to calculate the extrinsic and intrinsic contributions to the piezoelectricity in a single crystal of the ferroelectric PbZr 1− x Ti x O 3 ( x = 0.35). The root‐mean‐square value of the piezoelectric coefficient was obtained as 112 pC N −1 . The contribution of the domain‐wall motion is estimated as 99 pC N −1 . The contribution of electric‐field‐induced changes to the lattice parameters averaged over all the domains is 71 pC N −1 . The equivalent value corresponding to the change in lattice parameters in individual domains may reach up to 189 pC N −1 .