Domain wall excitations and their contributions to the weak‐signal response of doped lead zirconate titanate ceramics

1988 ◽  
Vol 64 (11) ◽  
pp. 6445-6451 ◽  
Author(s):  
Q. M. Zhang ◽  
W. Y. Pan ◽  
S. J. Jang ◽  
L. E. Cross
Keyword(s):  
Domain Wall ◽  
Lead Zirconate Titanate ◽  
Lead Zirconate ◽  
Weak Signal ◽  
Zirconate Titanate ◽  
Signal Response ◽  
Titanate Ceramics

De-aging of Fe-doped lead-zirconate-titanate ceramics by electric field cycling: 180°- vs. non-180° domain wall processes

2012 ◽  
Vol 112 (3) ◽  
pp. 034103 ◽  
Author(s):  
Julia Glaum ◽  
Yuri A. Genenko ◽  
Hans Kungl ◽  
Ljubomira Ana Schmitt ◽  
Torsten Granzow
Keyword(s):  
Domain Wall ◽  
Electric Field ◽  
Lead Zirconate Titanate ◽  
Lead Zirconate ◽  
Zirconate Titanate ◽  
Field Cycling ◽  
Titanate Ceramics

Evaluation of domain wall motion in lead zirconate titanate ceramics by nonlinear response measurements

2008 ◽  
Vol 103 (5) ◽  
pp. 054108 ◽  
Author(s):  
J. E. García ◽  
R. Pérez ◽  
D. A. Ochoa ◽  
A. Albareda ◽  
M. H. Lente ◽  
...  
Keyword(s):  
Domain Wall ◽  
Lead Zirconate Titanate ◽  
Nonlinear Response ◽  
Wall Motion ◽  
Domain Wall Motion ◽  
Lead Zirconate ◽  
Zirconate Titanate ◽  
Titanate Ceramics

Convergent-bceam diffraction studies on lead zirconate titanate Ceramics

1986 ◽  
Vol 44 ◽  
pp. 482-483
Author(s):  
M.L.A. Dass ◽  
T.A. Bielicki ◽  
G. Thomas ◽  
T. Yamamoto ◽  
K. Okazaki
Keyword(s):  
Lead Zirconate Titanate ◽  
Direct Proof ◽  
Lead Zirconate ◽  
Subsolidus Phase ◽  
Pzt Ceramics ◽  
Subsolidus Phase Diagram ◽  
Zirconate Titanate ◽  
Two Phases ◽  
Cbd Method ◽  
Titanate Ceramics

Lead zirconate titanate, Pb(Zr,Ti)O3 (PZT), ceramics are ferroelectrics formed as solid solutions between ferroelectric PbTiO3 and ant iferroelectric PbZrO3. The subsolidus phase diagram is shown in figure 1. PZT transforms between the Ti-rich tetragonal (T) and the Zr-rich rhombohedral (R) phases at a composition which is nearly independent of temperature. This phenomenon is called morphotropism, and the boundary between the two phases is known as the morphotropic phase boundary (MPB). The excellent piezoelectric and dielectric properties occurring at this composition are believed to.be due to the coexistence of T and R phases, which results in easy poling (i.e. orientation of individual grain polarizations in the direction of an applied electric field). However, there is little direct proof of the coexistence of the two phases at the MPB, possibly because of the difficulty of distinguishing between them. In this investigation a CBD method was found which would successfully differentiate between the phases, and this was applied to confirm the coexistence of the two phases.

Contribution from Ferroelastic Domain Switching Detected Using X-ray Diffraction toR-Curves in Lead Zirconate Titanate Ceramics

2001 ◽  
Vol 84 (12) ◽  
pp. 2921-2929 ◽  
Author(s):  
Alexandre E. Glazounov ◽  
Hans Kungl ◽  
Jan-Thorsten Reszat ◽  
Michael J. Hoffmann ◽  
Arnd Kolleck ◽  
...  
Keyword(s):  
Lead Zirconate Titanate ◽  
Domain Switching ◽  
Lead Zirconate ◽  
X Ray Diffraction ◽  
X Ray ◽  
Zirconate Titanate ◽  
Titanate Ceramics
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