Nonlinear electric field tuning characteristics of yttrium iron garnet–lead zirconate titanate microwave resonators

2008 ◽  
Vol 93 (3) ◽  
pp. 033508 ◽  
Author(s):  
Y. K. Fetisov ◽  
G. Srinivasan
Keyword(s):  
Electric Field ◽  
Lead Zirconate Titanate ◽  
Yttrium Iron Garnet ◽  
Lead Zirconate ◽  
Yttrium Iron ◽  
Microwave Resonators ◽  
Zirconate Titanate ◽  
Iron Garnet

ChemInform Abstract: Reaction Between Lead Zirconate Titanate and Yttrium Iron Garnet.

ChemInform ◽  
2010 ◽  
Vol 31 (18) ◽  
pp. no-no
Author(s):  
T. G. Lupeiko ◽  
I. V. Lisnevskaya ◽  
A. V. Chernyshev
Keyword(s):  
Lead Zirconate Titanate ◽  
Yttrium Iron Garnet ◽  
Lead Zirconate ◽  
Yttrium Iron ◽  
Zirconate Titanate ◽  
Iron Garnet

Reaction between lead zirconate titanate and yttrium iron garnet

2000 ◽  
Vol 36 (1) ◽  
pp. 84-85 ◽  
Author(s):  
T. G. Lupeiko ◽  
I. V. Lisnevskaya ◽  
A. V. Chernyshev
Keyword(s):  
Lead Zirconate Titanate ◽  
Yttrium Iron Garnet ◽  
Lead Zirconate ◽  
Yttrium Iron ◽  
Zirconate Titanate ◽  
Iron Garnet

Effects of exchange interactions on magnetoacoustic resonance in layered nanocomposites of yttrium iron garnet and lead zirconate titanate

2007 ◽  
Vol 22 (8) ◽  
pp. 2174-2178 ◽  
Author(s):  
O.V. Ryabkov ◽  
S.V. Averkin ◽  
M.I. Bichurin ◽  
V.M. Petrov ◽  
G. Srinivasan
Keyword(s):  
Lead Zirconate Titanate ◽  
Yttrium Iron Garnet ◽  
Mechanical Strain ◽  
Exchange Interactions ◽  
Lead Zirconate ◽  
Yttrium Iron ◽  
Magnetic Exchange ◽  
Zirconate Titanate ◽  
Piezoelectric Phase ◽  
Iron Garnet

In ferrite–piezoelectric bilayers, the magnetoelectric (ME) interaction is mediated by mechanical strain. The ME coupling is expected to be strong, particularly when the magnetic and electric subsystems show resonance. Here we address the effect of magnetic exchange interactions on ME coupling at magnetoacoustic resonance (MAR), i.e., at the coincidence of electromechanical resonance in the piezoelectric phase and ferromagnetic resonance in a tangentially magnetized ferrite. When exchange is ignored, the estimated ME coefficient versus frequency profile shows a giant magnetoelectric coefficient at MAR, about 75–100 V/cm Oe for yttrium–iron garnet (YIG)/lead zirconate–titanate (PZT) nano bilayers. The magnetic exchange is predicted to enhance the coupling at MAR and produce a secondary peak due to the excitation of magnetoacoustic modes. Estimates of the ME coefficient are provided as a function of thickness ratio of YIG and PZT.

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

Electric field forced phase switching in La‐modified lead zirconate titanate stannate thin films

1994 ◽  
Vol 75 (3) ◽  
pp. 1699-1704 ◽  
Author(s):  
K. G. Brooks ◽  
J. Chen ◽  
K. R. Udayakumar ◽  
L. E. Cross
Keyword(s):  
Thin Films ◽  
Electric Field ◽  
Lead Zirconate Titanate ◽  
Lead Zirconate ◽  
Phase Switching ◽  
Zirconate Titanate
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