Thickness Dependence of the Domain Structure in Thin BST Films

2015 ◽  
Vol 477 (1) ◽  
pp. 9-14
Author(s):  
A. N. Kuskova ◽  
O. M. Zhigalina ◽  
R. V. Gainutdinov
2020 ◽  
Vol 29 (9) ◽  
pp. 095019 ◽  
Author(s):  
Yuanzhi Xiang ◽  
Kun Liang ◽  
Scott Keller ◽  
Michael Guevara ◽  
Michael Sheng ◽  
...  

1963 ◽  
Vol 3 (11) ◽  
pp. 2101-2110 ◽  
Author(s):  
R. Gemperle ◽  
A. Gemperle ◽  
I. Bursuc

1994 ◽  
Vol 361 ◽  
Author(s):  
Kazuhide Abe ◽  
Shuichi Komatsu

ABSTRACTBa0.44Sr0.56TiO3 (BST) thin films with various thicknesses were epitaxially grown on Pt/MgO(100) substrates with rf magnetron sputtering. The thickness dependence of lattice constant, D-E hysteresis and dielectric constant were evaluated for the BST films. The lattice constant in the thickness direction is elongated through the thickness range (33 to 221 nm), whereas the ferroelectric and the dielectric properties had strong thickness dependencies. The mechanism of the induced ferroelectricity is discussed in terms of the thickness dependence and deposition technique.


Author(s):  
B. G. Demczyk

CoCr thin films have been of interest for a number of years due to their strong perpendicular anisotropy, favoring magnetization normal to the film plane. The microstructure and magnetic properties of CoCr films prepared by both rf and magnetron sputtering have been examined in detail. By comparison, however, relatively few systematic studies of the magnetic domain structure and its relation to the observed film microstructure have been reported. In addition, questions still remain as to the operative magnetization reversal mechanism in different film thickness regimes. In this work, the magnetic domain structure in magnetron sputtered Co-22 at.%Cr thin films of known microstructure were examined by Lorentz transmission electron microscopy. Additionally, domain nucleation studies were undertaken via in-situ heating experiments.It was found that the 50 nm thick films, which are comprised of columnar grains, display a “dot” type domain configuration (Figure 1d), characteristic of a perpendicular magnetization. The domain size was found to be on the order of a few structural columns in diameter.


Author(s):  
E.K. Goo ◽  
R.K. Mishra

Ferroelectric domains are twins that are formed when PZT undergoes a phase transformation from a non-ferroelectric cubic phase to a ferroelectric tetragonal phase upon cooling below ∼375°C.,1 The tetragonal phase is spontaneously polarized in the direction of c-axis, making each twin a ferroelectric domain. Thin foils of polycrystalline Pb (Zr.52Ti.48)03 were made by ion milling and observed in the Philips EM301 with a double tilt stage.


1981 ◽  
Vol 42 (C6) ◽  
pp. C6-825-C6-827
Author(s):  
P. Taborek ◽  
M. Sinvani ◽  
M. Weimer ◽  
D. Goodstein

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