Dynamic Response of the Electro-Optic Effect in Epitaxial Ferroelectric Thin Films

1999 ◽  
Vol 597 ◽  
Author(s):  
B. H. Hoerman ◽  
J. C. Majewski ◽  
B. M. Nichols ◽  
A. Teren ◽  
B. W. Wessels

AbstractThe dynamic response of the electro-optic coefficients and the electronic polarizability for epitaxial thin films of KnbO3 and BaTiO3 are measured. For these two systems a logarithmic dependence of the electro-optic response and the polarization on time was observed after removal of an applied electric field. The dynamic response of the electro-optic effect and the polarization of the films are attributed to the same physical mechanism, which we associate with the dynamic response of ferroelectric nanodomains.

2000 ◽  
Vol 655 ◽  
Author(s):  
C. S. Ganpule ◽  
A. L. Roytburd ◽  
V. Nagarajan ◽  
A. Stanishevsky ◽  
J. Melngailis ◽  
...  

AbstractFocused ion beam milling was used to fabricate ferroelectric islands in Pb-Zr-Ti-O thin films. The islands ranged in size from 200μm×200μm to 0.3μm×0.3μm. The inverse piezoelectric effect was studied in these islands as a function of their size by tracking the surface displacement of the top electrode of the island (under an applied electric field) using an atomic force microscope (AFM). It was found that there was a substantial increase in the piezoresponse as the size of the island decreased below 100μm×100μm. This increase was attributed to the elastic deformation of the substrate.


2014 ◽  
Vol 105 (11) ◽  
pp. 112903 ◽  
Author(s):  
Lei Chen ◽  
Yuan Zhang ◽  
Quan Guo ◽  
Dongwen Zhang ◽  
Xiangli Zhong ◽  
...  

2003 ◽  
Vol 784 ◽  
Author(s):  
A. K. Tagantsev ◽  
P. Muralt ◽  
J. Fousek

ABSTRACTA simple theory for the shape of the piezoelectric hysteresis loops (piezoelectric coefficient d vs. applied electric field E) is developed for the case of non-ferroelelastic 180° switching in ferroelectrics. The theory provides explanations for specific features of piezoelectric hysteresis loops, which have been observed in single crystals, thin films and in ceramics in particular. The piezoelectric coefficient may show a “hump”, i.e. when E decreases from the tip of the loop down to zero, d passes through a maximum, and a “nose”, i.e. a self-crossing of the loop close to its tips. The theory also explains the difference in the coercive fields seen in the polarization and piezoelectric loops.


2018 ◽  
Vol 123 (8) ◽  
pp. 084103 ◽  
Author(s):  
Ye Qiu ◽  
Huaping Wu ◽  
Jie Wang ◽  
Jia Lou ◽  
Zheng Zhang ◽  
...  

Author(s):  
Shinya Kondo ◽  
Reijiro Shimura ◽  
Takashi TERANISHI ◽  
Akira Kishimoto ◽  
Takanori Nagasaki ◽  
...  

1995 ◽  
Vol 11 (1-4) ◽  
pp. 69-80 ◽  
Author(s):  
G. Teowee ◽  
C. D. Baertlein ◽  
John T. Simpson ◽  
Tianji Zhao ◽  
M. Mansuripur ◽  
...  

2018 ◽  
Vol 23 ◽  
pp. 1-7
Author(s):  
Rabi Noori Hammudi ◽  
Sudad Salman Al-Bassam ◽  
Rawa Khalil Ibrahim ◽  
Aseel Ibrahim Mahmood ◽  
Peter Kopčanský ◽  
...  

In this work we have studied the electro-optical effect of two types of ferronematic nanoparticles. The first sample doped with magnetic material Fe3O4 and the second sample doped with a ferroelectric material SbSI. The difference in the two types of material that has been vaccinated led to different values of electro-optic properties because of the different susceptibility of materials. We have noticed that the material SbSI was more responsive to the applied electric field due to the nature of the constituent material (electric material) than the Fe3O4 ferromagnetic. The response time for the material SbSI is less than the response time of the ferromagnetic Fe3O4, that led to make the material SbSI best in the optical switch applications.


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