Graphene-lead zirconate titanate optothermal field effect transistors

2012 ◽  
Vol 100 (11) ◽  
pp. 113507 ◽  
Author(s):  
Chun-Yi Hsieh ◽  
Yung-Ting Chen ◽  
Wei-Jyun Tan ◽  
Yang-Fang Chen ◽  
Wan Y. Shih ◽  
...  
Keyword(s):  
Lead Zirconate Titanate ◽  
Field Effect ◽  
Field Effect Transistors ◽  
Lead Zirconate ◽  
Zirconate Titanate

Zno field-effect transistors with lead-zirconate-titanate ferroelectric gate

2015 ◽  
Vol 19 (sup2) ◽  
pp. S2-181-S2-184
Author(s):  
X. Zhang ◽  
D. Xie ◽  
J. Xu ◽  
C. Zhang ◽  
Y. Sun ◽  
...  
Keyword(s):  
Lead Zirconate Titanate ◽  
Field Effect ◽  
Field Effect Transistors ◽  
Lead Zirconate ◽  
Zirconate Titanate

MoS2 Field-Effect Transistors With Lead Zirconate-Titanate Ferroelectric Gating

2015 ◽  
Vol 36 (8) ◽  
pp. 784-786 ◽  
Author(s):  
Xiao-Wen Zhang ◽  
Dan Xie ◽  
Jian-Long Xu ◽  
Yi-Lin Sun ◽  
Xian Li ◽  
...  
Keyword(s):  
Lead Zirconate Titanate ◽  
Field Effect ◽  
Field Effect Transistors ◽  
Lead Zirconate ◽  
Zirconate Titanate

scholarly journals Fabrication and current-voltage characterization of a ferroelectric lead zirconate titanate/AlGaN∕GaN field effect transistor

2006 ◽  
Vol 88 (12) ◽  
pp. 123508 ◽  
Author(s):  
Youn-Seon Kang ◽  
Qian Fan ◽  
Bo Xiao ◽  
Ya. I. Alivov ◽  
Jinqiao Xie ◽  
...  
Keyword(s):  
Lead Zirconate Titanate ◽  
Field Effect ◽  
Field Effect Transistor ◽  
Lead Zirconate ◽  
Zirconate Titanate ◽  
Current Voltage ◽  
Effect Transistor

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.

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