Formation, Atomic Structures and Properties of Carbon Nanocage Materials

2006 ◽  
pp. 187-216 ◽  
Author(s):  
Takeo Oku ◽  
Ichihito Narita ◽  
Atsushi Nishiwaki ◽  
Naruhiro Koi ◽  
Katsuaki Suganuma ◽  
...  
2004 ◽  
Vol 10 (S02) ◽  
pp. 6-7 ◽  
Author(s):  
Yuichi Ikuhara

Extended abstract of a paper presented at Microscopy and Microanalysis 2004 in Savannah, Georgia, USA, August 1–5, 2004.


2000 ◽  
Vol 74 (1-3) ◽  
pp. 206-217 ◽  
Author(s):  
Takeo Oku ◽  
Takanori Hirano ◽  
Masaki Kuno ◽  
Takafumi Kusunose ◽  
Koichi Niihara ◽  
...  

2013 ◽  
Vol 779-780 ◽  
pp. 239-242
Author(s):  
Fan Wang ◽  
Xing Yu Zhao ◽  
Lei Cui

Atomic structures and properties of Ni nanowires are studied by using the generalized simulated annealing method with SuttonChen potential. Amorphous-like, helical, face-centered cubic and defect structures are found for different wire lengths. And from the analyses of the binding energy and angular correlation function (ACF), it is found that the helical structure of the Ni nanowires is the most stable form. With the compression and extension, the nanowires could transform from fcc [11 structure to fcc [110] one.


2008 ◽  
Vol 584-586 ◽  
pp. 41-48 ◽  
Author(s):  
Herbert Gleiter

Recently, a new class of materials - called nanoglasses - with a glassy structure was synthesized. The novel feature of these materials is that the atomic structure in the entire volume of the material as well as the density of the material can be tuned. Nanoglasses are generated by introducing interfaces into metallic glasses on a nanometer scale. Interfaces in these nanoglasses delocalize upon annealing, so that the free volume associated with these interfaces spreads throughout the volume of the glass. This delocalization changes the atomic structure and the density of the glass throughout the volume. In fact, by controlling the spacing between the interfaces introduced into the glass as well as the degree of the delocalization (by modifying the annealing time and/or annealing temperature), the atomic structures as well as the density (and hence all structure/density dependent properties) of nanoglasses may be controlled. A comparable tuning of the atomic structure/density of crystalline materials is not conceivable, because defects in crystals do not delocalize upon annealing.


2010 ◽  
Vol 16 (S2) ◽  
pp. 1466-1467
Author(s):  
Y Ikuhara ◽  
Y Sato ◽  
SD Findlay ◽  
T Mizoguchi ◽  
N Shibata ◽  
...  

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


2012 ◽  
Vol 18 (S2) ◽  
pp. 524-525 ◽  
Author(s):  
S. Bals ◽  
B. Goris ◽  
G. Van Tendeloo

Extended abstract of a paper presented at Microscopy and Microanalysis 2012 in Phoenix, Arizona, USA, July 29 – August 2, 2012.


Author(s):  
D. Cherns

The use of high resolution electron microscopy (HREM) to determine the atomic structure of grain boundaries and interfaces is a topic of great current interest. Grain boundary structure has been considered for many years as central to an understanding of the mechanical and transport properties of materials. Some more recent attention has focussed on the atomic structures of metalsemiconductor interfaces which are believed to control electrical properties of contacts. The atomic structures of interfaces in semiconductor or metal multilayers is an area of growing interest for understanding the unusual electrical or mechanical properties which these new materials possess. However, although the point-to-point resolutions of currently available HREMs, ∼2-3Å, appear sufficient to solve many of these problems, few atomic models of grain boundaries and interfaces have been derived. Moreover, with a new generation of 300-400kV instruments promising resolutions in the 1.6-2.0 Å range, and resolutions better than 1.5Å expected from specialist instruments, it is an appropriate time to consider the usefulness of HREM for interface studies.


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