biaxial texture
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2016 ◽  
Vol 45 (7) ◽  
pp. 3546-3553 ◽  
Author(s):  
Yan Xue ◽  
Ya-Hui Zhang ◽  
Rui-Peng Zhao ◽  
Fei Zhang ◽  
Yu-Ming Lu ◽  
...  

Author(s):  
James R. Groves ◽  
Robert H. Hammond ◽  
Vladimir Matias ◽  
Raymond F. DePaula ◽  
Liliana Stan ◽  
...  

2012 ◽  
Vol 338 (1) ◽  
pp. 118-124 ◽  
Author(s):  
T. Roch ◽  
E. Dobročka ◽  
M. Mikula ◽  
A. Pidík ◽  
P. Durina ◽  
...  

2011 ◽  
Vol 519 (16) ◽  
pp. 5413-5418 ◽  
Author(s):  
P. Snow ◽  
C. Gaire ◽  
T.-M. Lu ◽  
G.-C. Wang

2011 ◽  
Vol 1308 ◽  
Author(s):  
Gwo-Ching Wang ◽  
Yu Liu ◽  
Churamani Gaire ◽  
Wen Yuan ◽  
Toh-Ming Lu

ABSTRACTThe most frequently used characterization technique for biaxial texture formation in thin films is x-ray pole figure analysis. However, x-rays interact weakly with matter and can penetrate a few microns deep into the film. The texture obtained by x-rays is therefore an average texture from the entire thickness of the film. As the texture of a film often changes during growth, information on the basic mechanisms that control the final texture is often lost. In contrast electrons interact strongly with matter and they have very limited penetration and escape depths of a few nm. In this paper we will show how we can use our newly developed reflection high energy electron diffraction (RHEED) surface pole figure technique to probe the surface texture evolution of the growth front from the initial stage (nm thick) to the later stage. The RHEED pole figure technique is a surface-sensitive technique that allows us to obtain information on the dynamic behavior of texture evolution of the growth front during film deposition. We shall explain the principle, measurement, and construction of such RHEED surface pole figures. An example of the biaxial texture evolution of CaF2 due to the atomic shadowing effect during oblique angle deposition is described.


2010 ◽  
Vol 1254 ◽  
Author(s):  
James Groves ◽  
Robert Hammond ◽  
Vladimir Matias ◽  
Liliana Stan ◽  
Raymond F DePaula ◽  
...  

AbstractRecent efforts in investigating the mechanism of ion beam assisted deposition (IBAD) of biaxially textured thin films of magnesium oxide (MgO) template layers have shown that the texture develops suddenly during the initial 2 nm of deposition. To help understand and tune the behavior during this initial stage, we pre-deposited thin layers of MgO with no ion assist prior to IBAD growth of MgO. We found that biaxial texture develops for pre-deposited thicknesses < 2 nm, and that the thinnest layer tested, at 1 nm, resulted in the best qualitative RHEED image, indicative of good biaxial texture development. The texture developed during IBAD growth on the 1.5 nm pre-deposited layer is slightly worse and IBAD growth on the 2 nm pre-deposited layer produces a fiber texture. Application of these layers on an Al2O3 starting surface, which has been shown to impede texture development, improves the overall quality of the IBAD MgO and has some of the characteristics of a biaxially texture RHEED pattern. It is suggested that the use of thin (<2 nm) pre-deposited layers may eliminate the need for bed layers like Si3N4 and Y2O3 that are currently thought to be required for proper biaxial texture development in IBAD MgO.


2009 ◽  
Vol 1184 ◽  
Author(s):  
Fu Tang ◽  
Toh-Ming Lu ◽  
Gwo Ching Wang

AbstractIn this report we present a brief overview of the growth of nanostructures by the oblique angle deposition where the nanostructures possess both out-of-plane and in-plane preferred orientations or a biaxial texture. The degree of preferred crystal orientations can be quantitatively determined from a method called “RHEED surface pole figure analysis” that we developed recently.


2009 ◽  
Vol 24 (1) ◽  
pp. 125-129 ◽  
Author(s):  
Vladimir Matias ◽  
Jens Hänisch ◽  
E. John Rowley ◽  
Konrad Güth

We examined crystalline-texture evolution during ion-beam-assisted deposition (IBAD) of MgO thin films. We have demonstrated for the first time that in-plane crystalline texturing in IBAD of MgO scales with deposition rate. At high ion currents an in-plane texture full width at half-maximum (FWHM) of 10° can be achieved in less than 1 s, and 6° in 2.2 s. MgO texture further improves with thickness of a homoepitaxial layer deposited on top. We have developed an empirical quantification of the texture evolution in both IBAD and homoepitaxial layers. The best texture attained thus far in the MgO layer on polished Hastelloy tape has an in-plane FWHM of 1.6°. The high deposition rates demonstrated here make high-throughput manufacturing of IBAD textured templates a practical and cost-effective concept.


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