scholarly journals Deuterium uptake and sputtering of simultaneous lithiated, boronized, and oxidized carbon surfaces irradiated by low-energy deuterium

2018 ◽  
Vol 123 (19) ◽  
pp. 195901 ◽  
Author(s):  
F. J. Domínguez-Gutiérrez ◽  
P. S. Krstić ◽  
J. P. Allain ◽  
F. Bedoya ◽  
M. M. Islam ◽  
...  
Keyword(s):  
Low Energy ◽  
Deuterium Uptake ◽  
Oxidized Carbon ◽  
Carbon Surfaces

scholarly journals Effects of roughness and temperature on low-energy hydrogen positive and negative ion reflection from silicon and carbon surfaces

2014 ◽  
Vol 85 (2) ◽  
pp. 02C311 ◽  
Author(s):  
N. Tanaka ◽  
S. Kato ◽  
T. Miyamoto ◽  
M. Nishiura ◽  
K. Tsumori ◽  
...  
Keyword(s):  
Low Energy ◽  
Negative Ion ◽  
Carbon Surfaces

Interaction of Low-Energy Ions and Hydrocarbon Radicals with Carbon Surfaces

ChemInform ◽  
2006 ◽  
Vol 37 (25) ◽  
Author(s):  
W. Jacob ◽  
C. Hopf ◽  
M. Meier ◽  
T. Schwarz-Selinger
Keyword(s):  
Low Energy ◽  
Hydrocarbon Radicals ◽  
Carbon Surfaces ◽  
Low Energy Ions

Dissociated Σ=27 boundaries in silicon

1988 ◽  
Vol 46 ◽  
pp. 624-625
Author(s):  
A. Garg ◽  
W.A.T. Clark ◽  
J.P. Hirth
Keyword(s):  
Electron Diffraction ◽  
Local Minimum ◽  
Boundary Energy ◽  
Coincidence Site Lattice ◽  
Boundary Plane ◽  
Low Energy ◽  
Theoretical Understanding ◽  
Site Lattice ◽  
Kikuchi Pattern ◽  
Analysis Techniques

In the last twenty years, a significant amount of work has been done in the theoretical understanding of grain boundaries. The various proposed grain boundary models suggest the existence of coincidence site lattice (CSL) boundaries at specific misorientations where a periodic structure representing a local minimum of energy exists between the two crystals. In general, the boundary energy depends not only upon the density of CSL sites but also upon the boundary plane, so that different facets of the same boundary have different energy. Here we describe TEM observations of the dissociation of a Σ=27 boundary in silicon in order to reduce its surface energy and attain a low energy configuration.The boundary was identified as near CSL Σ=27 {255} having a misorientation of (38.7±0.2)°/[011] by standard Kikuchi pattern, electron diffraction and trace analysis techniques. Although the boundary appeared planar, in the TEM it was found to be dissociated in some regions into a Σ=3 {111} and a Σ=9 {122} boundary, as shown in Fig. 1.

Transfer optics for high spatial resolution electron spectroscopy

1988 ◽  
Vol 46 ◽  
pp. 666-667
Author(s):  
G. G. Hembree ◽  
Luo Chuan Hong ◽  
P.A. Bennett ◽  
J.A. Venables
Keyword(s):  
Magnetic Field ◽  
Scanning Transmission Electron Microscope ◽  
Low Energy ◽  
Objective Lens ◽  
State University ◽  
Arizona State University ◽  
Initial Field ◽  
Resolution Electron ◽  
Scanning Transmission ◽  
Low Energy Electrons

A new field emission scanning transmission electron microscope has been constructed for the NSF HREM facility at Arizona State University. The microscope is to be used for studies of surfaces, and incorporates several surface-related features, including provision for analysis of secondary and Auger electrons; these electrons are collected through the objective lens from either side of the sample, using the parallelizing action of the magnetic field. This collimates all the low energy electrons, which spiral in the high magnetic field. Given an initial field Bi∼1T, and a final (parallelizing) field Bf∼0.01T, all electrons emerge into a cone of semi-angle θf≤6°. The main practical problem in the way of using this well collimated beam of low energy (0-2keV) electrons is that it is travelling along the path of the (100keV) probing electron beam. To collect and analyze them, they must be deflected off the beam path with minimal effect on the probe position.

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