Position dependence of the visibility of a single gold atom in silicon crystals in HAADF-STEM image simulation

1997 ◽  
Vol 46 (1) ◽  
pp. 33-43 ◽  
Author(s):  
K. Nakamura ◽  
H. Kakibayashi ◽  
K. Kanehori ◽  
N. Tanaka
Author(s):  
E. J. Kirkland

In a STEM an electron beam is focused into a small probe on the specimen. This probe is raster scanned across the specimen to form an image from the electrons transmitted through the specimen. The objective lens is positioned before the specimen instead of after the specimen as in a CTEM. Because the probe is focused and scanned before the specimen, accurate annular dark field (ADF) STEM image simulation is more difficult than CTEM simulation. Instead of an incident uniform plane wave, ADF-STEM simulation starts with a probe wavefunction focused at a specified position on the specimen. The wavefunction is then propagated through the specimen one atomic layer (or slice) at a time with Fresnel diffraction between slices using the multislice method. After passing through the specimen the wavefunction is diffracted onto the detector. The ADF signal for one position of the probe is formed by integrating all electrons scattered outside of an inner angle large compared with the objective aperture.


2014 ◽  
Vol 20 (S3) ◽  
pp. 154-155 ◽  
Author(s):  
Michael Odlyzko ◽  
K. Andre Mkhoyan

Micron ◽  
2015 ◽  
Vol 74 ◽  
pp. 47-53 ◽  
Author(s):  
D.S. He ◽  
Z.Y. Li ◽  
J. Yuan

2009 ◽  
Vol 109 (9) ◽  
pp. 1203-1209 ◽  
Author(s):  
Takao Morimura ◽  
Masayuki Hasaka

Author(s):  
R. F. Loane

The multislice method has been adapted to simulate annular dark field (ADF) scanning transmission electron microscope (STEM) images. In the STEM image simulation, a highly focused electron probe is scanned across a specimen and the scattered intensity, accumulated over an annular detector, is recorded as a function of probe position. Each pixel in the STEM image is determined by an entire multislice calculation for a particular position of the incident probe. This N4 process is very computationally expensive and currently requires the use of a supercomputer to achieve runtimes of less than a day.The simulated specimen consisted of a (111) silicon crystal substrate, which was a multiple of 94 Å (30 slices) thick, followed by an additional slice containing a single gold atom. Slice potentials were 38.4 Å x 39.9 Å (256 x 256 pixels) in size, which set the maximum included scattering angle to 79 mrad.


2010 ◽  
Vol 16 (S2) ◽  
pp. 252-253
Author(s):  
BN Patrick ◽  
LF Allard ◽  
Y Shao-Horn ◽  
PJ Ferreira

Extended abstract of a paper presented at Microscopy and Microanalysis 2010 in Portland, Oregon, USA, August 1 – August 5, 2010.


Author(s):  
Takashi Yamazaki ◽  
Kazuto Watanabe ◽  
Koji Kuramochi ◽  
Iwao Hashimoto

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