Is there a perfect SiC MosFETs Device on an imperfect crystal?

Author(s):  
T. Neyer ◽  
M. Domeij ◽  
H. Das ◽  
S. Sunkari
Keyword(s):  
Author(s):  
S. Nakahara ◽  
D. M. Maher

Since Head first demonstrated the advantages of computer displayed theoretical intensities from defective crystals, computer display techniques have become important in image analysis. However the computational methods employed resort largely to numerical integration of the dynamical equations of electron diffraction. As a consequence, the interpretation of the results in terms of the defect displacement field and diffracting variables is difficult to follow in detail. In contrast to this type of computational approach which is based on a plane-wave expansion of the excited waves within the crystal (i.e. Darwin representation ), Wilkens assumed scattering of modified Bloch waves by an imperfect crystal. For localized defects, the wave amplitudes can be described analytically and this formulation has been used successfully to predict the black-white symmetry of images arising from small dislocation loops.


2010 ◽  
Vol 1 ◽  
pp. 24-47 ◽  
Author(s):  
Ulf Wiedwald ◽  
Luyang Han ◽  
Johannes Biskupek ◽  
Ute Kaiser ◽  
Paul Ziemann

Monatomic (Fe, Co) and bimetallic (FePt and CoPt) nanoparticles were prepared by exploiting the self-organization of precursor loaded reverse micelles. Achievements and limitations of the preparation approach are critically discussed. We show that self-assembled metallic nanoparticles can be prepared with diameters d = 2–12 nm and interparticle distances D = 20–140 nm on various substrates. Structural, electronic and magnetic properties of the particle arrays were characterized by several techniques to give a comprehensive view of the high quality of the method. For Co nanoparticles, it is demonstrated that magnetostatic interactions can be neglected for distances which are at least 6 times larger than the particle diameter. Focus is placed on FePt alloy nanoparticles which show a huge magnetic anisotropy in the L10 phase, however, this is still less by a factor of 3–4 when compared to the anisotropy of the bulk counterpart. A similar observation was also found for CoPt nanoparticles (NPs). These results are related to imperfect crystal structures as revealed by HRTEM as well as to compositional distributions of the prepared particles. Interestingly, the results demonstrate that the averaged effective magnetic anisotropy of FePt nanoparticles does not strongly depend on size. Consequently, magnetization stability should scale linearly with the volume of the NPs and give rise to a critical value for stability at ambient temperature. Indeed, for diameters above 6 nm such stability is observed for the current FePt and CoPt NPs. Finally, the long-term conservation of nanoparticles by Au photoseeding is presented.


1997 ◽  
Vol 04 (05) ◽  
pp. 985-990
Author(s):  
AYAHIKO ICHIMIYA ◽  
YUSUKE OHNO

For dynamical calculations of reflection high-energy electron diffraction (RHEED) for imperfect crystal surfaces, a general formula of Fourier coefficients of crystal potential with domain structures is developed. Using the formula, RHEED intensity rocking curves are calculated for a [Formula: see text]-Ag surface with antiphase domains. We discuss effects of antiphase domains of surfaces in structure determinations by RHEED.


1982 ◽  
Vol 45 (1) ◽  
pp. 19-23
Author(s):  
A. P. Levanyuk ◽  
G. M. Levanyuk ◽  
A. S. Sigov

RSC Advances ◽  
2015 ◽  
Vol 5 (98) ◽  
pp. 80749-80755 ◽  
Author(s):  
Xinggang Chen ◽  
Shuyan Shan ◽  
Jiayu Liu ◽  
Xiongwei Qu ◽  
Qingxin Zhang

o-BDB, m-BDB and p-BDB monomers with imperfect crystal structures were synthesized by a nucleophilic substitution reaction.


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