hrem image
Recently Published Documents


TOTAL DOCUMENTS

63
(FIVE YEARS 0)

H-INDEX

9
(FIVE YEARS 0)

2011 ◽  
Vol 20 (3) ◽  
pp. 213
Author(s):  
Patricia Donnadieu ◽  
Kenji Matsuda ◽  
Thierry Epicier ◽  
Joel Douin

Owing the phase image method (Hytch, 1998), strain fields can be derived from HREM images. The method is here applied to the nanoscale precipitates responsible for hardening in Aluminum alloys. Since the method is a very sensitive one, we have examined the impact of several aspects of the image quality (noise, fluctuations, distortion). The strain field information derived from the HREM image analysis is further introduced in a simulation of the dislocation motion in the matrix.


2005 ◽  
Vol 104 (3-4) ◽  
pp. 271-280 ◽  
Author(s):  
L.Y. Chang ◽  
R.R. Meyer ◽  
A.I. Kirkland

2004 ◽  
Vol 839 ◽  
Author(s):  
J. R. Jinschek ◽  
H. A. Calderon ◽  
K. J. Batenburg ◽  
V. Radmilovic ◽  
Ch. Kisielowski

ABSTRACTLow-resolution tomography requires recording images every few degrees. As a consequence, the sample is often degraded after such a procedure. However the required input can be reduced drastically by using knowledge about the position and the number of atoms in each atomic column. This concept has been tested in the present investigation where HREM image simulation (MacTempas) together with exit wave reconstruction (FEI Trueimage) have been performed. A cubeoctahedral nanoparticle is used for the simulation with different compositions i.e., pure solid Ga and In-Ga particles. Six different zone axes ([111], [111], [001], [110], [110], [011]) have been used and the parameters of an aberration corrected microscope (200kV, Cs = 0 mm, resolution = 0.5Å). The discrete grid data were determined by constructing a channeling map from the reconstructed exit wave images. In this special case only three projections [001], [110], [110] were sufficient to find a unique volumetric reconstruction, illustrating the potential of the method. The other projections were used for checking the solution. The comparison between the projected potentials (simulated input) and the final result shows that discrete tomography reconstructs the exact position of all 309 atoms and the three-dimensional shape of the nanocrystal.


2004 ◽  
Vol 839 ◽  
Author(s):  
B.G. Mendis ◽  
Y. Mishin ◽  
C.S. Hartley ◽  
K.J. Hemker

ABSTRACTQuantitative High Resolution Electron Microscopy (HREM) is used to characterize the in-plane displacements of atoms around a screw dislocation core in bcc molybdenum. The in-plane displacements have an important effect on the bulk mechanical properties of bcc metals and alloys. However, the largest displacements are predicted to be less than 10 pm, requiring that the atom positions in an HREM image be determined to sub-pixel accuracy. In order to calculate the displacements the positions of the atom columns in the undistorted crystal must be determined precisely from the information available in the HREM image. An algorithm for such a task is briefly discussed and the technique applied to several HREM images. It is seen that the atomic displacements are predominantly due to surface relaxation (i.e. Eshelby twist) of a thin TEM foil, thereby masking the finer displacements of the dislocation core. Nye tensor plots, which map the resultant Burgers vector at each point of a distorted crystal, are also used to characterize the core structure. Although the large displacements from the Eshelby twist were completely removed, no signal from the dislocation core region was observed.


2003 ◽  
Vol 94 (4) ◽  
pp. 358-367 ◽  
Author(s):  
G. Möbus ◽  
A. Levay ◽  
B. J. Inkson ◽  
M. J. Hÿtch ◽  
A. Trampert ◽  
...  
Keyword(s):  

2002 ◽  
Vol 25 (3) ◽  
pp. 413-426 ◽  
Author(s):  
J.A Ascencio ◽  
V Rodrı́guez-Lugo ◽  
C Angeles ◽  
T Santamarı́a ◽  
V.M Castaño

2000 ◽  
Vol 222 (1) ◽  
pp. 185-198 ◽  
Author(s):  
R. Hillebrand ◽  
H. Kirschner ◽  
P. Werner ◽  
U. G�sele

Sign in / Sign up

Export Citation Format

Share Document