Domain wall pinning by point defects in ferroelectric materials

Author(s):  
D. Schrade ◽  
R. Mueller ◽  
B. X. Xu ◽  
D. Gross
1986 ◽  
Vol 82 ◽  
Author(s):  
O. Boser ◽  
D. N. Beshers

ABSTRACTDopants in ferroelectric materials affect the dielectric constant and the shape of the hysteresis loop. To understand and quantify these effects it is necessary to calculate the interaction between dopant and domain wall. In the following the dopant ion is modelled as an elastic dipole. The stresses surrounding a 180° domain wall are calculated in analogy to calculations in the magnetic case for Bloch walls. It is assumed that electrostrictive effects control the strains and that the spontaneous polarization does not rotate but decreases to zero at the center of the domain wall and increases in the opposite direction on the other side of the domain wall. The calculations are made assumingisotropic elastic constants. It is found that only elastic dipoles oriented in the planeof the domain wall interact with it. The interaction forces as a function of perpendicular distance between wall and dipole show an antisymmetric characteristic.


1984 ◽  
Vol 44 (1-2) ◽  
pp. 187-194 ◽  
Author(s):  
A.E. Borovik ◽  
S. Klama ◽  
S.I. Kulinich

Author(s):  
Wenwu Cao

Domain structures play a key role in determining the physical properties of ferroelectric materials. The formation of these ferroelectric domains and domain walls are determined by the intrinsic nonlinearity and the nonlocal coupling of the polarization. Analogous to soliton excitations, domain walls can have high mobility when the domain wall energy is high. The domain wall can be describes by a continuum theory owning to the long range nature of the dipole-dipole interactions in ferroelectrics. The simplest form for the Landau energy is the so called ϕ model which can be used to describe a second order phase transition from a cubic prototype,where Pi (i =1, 2, 3) are the components of polarization vector, α's are the linear and nonlinear dielectric constants. In order to take into account the nonlocal coupling, a gradient energy should be included, for cubic symmetry the gradient energy is given by,


2005 ◽  
Vol 97 (10) ◽  
pp. 10E317 ◽  
Author(s):  
H. Asada ◽  
H. Ii ◽  
J. Yamasaki ◽  
M. Takezawa ◽  
T. Koyanagi

1990 ◽  
Vol 65 (24) ◽  
pp. 3025-3028 ◽  
Author(s):  
K. S. Liang ◽  
K. L. D’Amico ◽  
C. H. Lee ◽  
E. Y. Sheu

2010 ◽  
Vol 96 (2) ◽  
pp. 022501 ◽  
Author(s):  
R. Lavrijsen ◽  
G. Malinowski ◽  
J. H. Franken ◽  
J. T. Kohlhepp ◽  
H. J. M. Swagten ◽  
...  

2019 ◽  
Vol 475 ◽  
pp. 70-75 ◽  
Author(s):  
Tianli Jin ◽  
Funan Tan ◽  
Wai Cheung Law ◽  
Weiliang Gan ◽  
Ivan Soldatov ◽  
...  

2003 ◽  
Vol 52 (3) ◽  
pp. 708
Author(s):  
Rong Chuan-Bing ◽  
Zhang Hong-Wei ◽  
Zhang Jian ◽  
Zhang Shao-Ying ◽  
Shen Bao-Gen

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