Raman study of structural transformations of titania coatings induced by laser annealing

1984 ◽  
Vol 45 (10) ◽  
pp. 1065-1067 ◽  
Author(s):  
L. S. Hsu ◽  
R. Solanki ◽  
G. J. Collins ◽  
C. Y. She
2017 ◽  
Vol 48 (11) ◽  
pp. 1401-1405 ◽  
Author(s):  
Pavel S. Zelenovskiy ◽  
Anton O. Davydov ◽  
Alexander S. Krylov ◽  
Andrei L. Kholkin

1995 ◽  
Vol 52 (18) ◽  
pp. 13652-13657 ◽  
Author(s):  
V. G. Ivanov ◽  
M. N. Iliev ◽  
C. Thomsen

2013 ◽  
Vol 117 (43) ◽  
pp. 11006-11012 ◽  
Author(s):  
Gayatri Kumari ◽  
Kolleboyina Jayaramulu ◽  
Tapas Kumar Maji ◽  
Chandrabhas Narayana

1991 ◽  
Vol 69 (11) ◽  
pp. 7815-7819 ◽  
Author(s):  
H. S. Mavi ◽  
A. K. Shukla ◽  
K. P. Jain ◽  
S. C. Abbi ◽  
R. Beserman
Keyword(s):  
Cw Laser ◽  

2010 ◽  
Vol 93 (11) ◽  
pp. 3745-3751 ◽  
Author(s):  
Ralf Brüning ◽  
Justine B. Galbraith ◽  
Katherine E. Braedley ◽  
Jonathan Johnstone ◽  
Jacques Robichaud ◽  
...  

Author(s):  
Yu. M. Azhniuk ◽  
A. V. Gomonnai ◽  
V. V. Lopushansky ◽  
O. O. Gomonnai ◽  
V. M. Rubish ◽  
...  

Author(s):  
Jean-Luc Rouvière ◽  
Alain Bourret

The possible structural transformations during the sample preparations and the sample observations are important issues in electron microscopy. Several publications of High Resolution Electron Microscopy (HREM) have reported that structural transformations and evaporation of the thin parts of a specimen could happen in the microscope. Diffusion and preferential etchings could also occur during the sample preparation.Here we report a structural transformation of a germanium Σ=13 (510) [001] tilt grain boundary that occurred in a medium-voltage electron microscopy (JEOL 400KV).Among the different (001) tilt grain boundaries whose atomic structures were entirely determined by High Resolution Electron Microscopy (Σ = 5(310), Σ = 13 (320), Σ = 13 (510), Σ = 65 (1130), Σ = 25 (710) and Σ = 41 (910), the Σ = 13 (510) interface is the most interesting. It exhibits two kinds of structures. One of them, the M-structure, has tetracoordinated covalent bonds and is periodic (fig. 1). The other, the U-structure, is also tetracoordinated but is not strictly periodic (fig. 2). It is composed of a periodically repeated constant part that separates variable cores where some atoms can have several stable positions. The M-structure has a mirror glide symmetry. At Scherzer defocus, its HREM images have characteristic groups of three big white dots that are distributed on alternatively facing right and left arcs (fig. 1). The (001) projection of the U-structure has an apparent mirror symmetry, the portions of good coincidence zones (“perfect crystal structure”) regularly separate the variable cores regions (fig. 2).


1993 ◽  
Vol 3 (4) ◽  
pp. 1007-1029 ◽  
Author(s):  
M. Krauzman ◽  
A. Colline ◽  
D. Kirin ◽  
R. M. Pick ◽  
N. Toupry

1981 ◽  
Vol 42 (C4) ◽  
pp. C4-903-C4-906 ◽  
Author(s):  
A. P. Firth ◽  
A. E. Owen ◽  
P. J. Ewen
Keyword(s):  

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