Field‐induced strains and polarization switching mechanisms in La‐modified lead zirconate titanate ceramics

1996 ◽  
Vol 79 (4) ◽  
pp. 2023-2028 ◽  
Author(s):  
Xunhu Dai ◽  
Z. Xu ◽  
Jie‐Fang Li ◽  
Dwight Viehland
2010 ◽  
Vol 108 (1) ◽  
pp. 014105 ◽  
Author(s):  
Sergey Zhukov ◽  
Sergey Fedosov ◽  
Julia Glaum ◽  
Torsten Granzow ◽  
Yuri A. Genenko ◽  
...  

Author(s):  
M.L.A. Dass ◽  
T.A. Bielicki ◽  
G. Thomas ◽  
T. Yamamoto ◽  
K. Okazaki

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.


2001 ◽  
Vol 84 (12) ◽  
pp. 2921-2929 ◽  
Author(s):  
Alexandre E. Glazounov ◽  
Hans Kungl ◽  
Jan-Thorsten Reszat ◽  
Michael J. Hoffmann ◽  
Arnd Kolleck ◽  
...  

2012 ◽  
Vol 41 (3) ◽  
pp. 156-163 ◽  
Author(s):  
Rafael Hernández García ◽  
Moni Behar ◽  
Johnny Ferraz Dias ◽  
Margarita Edelia Villanueva Tagle ◽  
María Dolores Durruthy Rodríguez ◽  
...  

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