scholarly journals In-Plane Stacking Disorder in Polydisperse Hard Sphere Crystals

Langmuir ◽  
2007 ◽  
Vol 23 (7) ◽  
pp. 3554-3560 ◽  
Author(s):  
Janne-Mieke Meijer ◽  
Volkert W. A. de Villeneuve ◽  
Andrei V. Petukhov
Keyword(s):  
Hard Sphere ◽  
Stacking Disorder

Succession of stacking disorder in hard-sphere crystal under gravity by Monte Carlo simulation

2007 ◽  
Vol 257 (2) ◽  
pp. 131-138 ◽  
Author(s):  
Atsushi Mori ◽  
Yoshihisa Suzuki ◽  
Shin-ichiro Yanagiya
Keyword(s):  
Monte Carlo Simulation ◽  
Monte Carlo ◽  
Hard Sphere ◽  
Stacking Disorder

Monte Carlo simulations of in-plane stacking disorder in hard-sphere crystals

2008 ◽  
Vol 77 (1) ◽  
Author(s):  
P. S. Miedema ◽  
V. W. A. de Villeneuve ◽  
A. V. Petukhov
Keyword(s):  
Monte Carlo ◽  
Monte Carlo Simulations ◽  
Hard Sphere ◽  
Stacking Disorder

“Preparation of Single Crystalline Gold Films for ED Studies”

1972 ◽  
Vol 30 ◽  
pp. 634-635
Author(s):  
Joseph D. C. Peng
Keyword(s):  
Crystal Morphology ◽  
Diffraction Theory ◽  
Scattering Matrix ◽  
Vacuum Evaporation ◽  
Gold Films ◽  
Matrix Formulation ◽  
Silver Films ◽  
Single Crystalline ◽  
Grating Pattern ◽  
Stacking Disorder

The relative intensities of the ED spots in a cross-grating pattern can be calculated using N-beam electron diffraction theory. The scattering matrix formulation of N-beam ED theory has been previously applied to imperfect microcrystals of gold containing stacking disorder (coherent twinning) in the (111) crystal plane. In the present experiment an effort has been made to grow single-crystalline, defect-free (111) gold films of a uniform and accurately know thickness using vacuum evaporation techniques. These represent stringent conditions to be met experimentally; however, if a meaningful comparison is to be made between theory and experiment, these factors must be carefully controlled. It is well-known that crystal morphology, perfection, and orientation each have pronounced effects on relative intensities in single crystals.The double evaporation method first suggested by Pashley was employed with some modifications. Oriented silver films of a thickness of about 1500Å were first grown by vacuum evaporation on freshly cleaved mica, with the substrate temperature at 285° C during evaporation with the deposition rate at 500-800Å/sec.

The screened Coulomb (Yukawa) charged hard sphere binary fluid

1997 ◽  
Vol 92 (2) ◽  
pp. 211-228 ◽  
Author(s):  
R.J. F. LEOTE DE CARVALHO ◽  
R. EVANS
Keyword(s):  
Hard Sphere ◽  
Binary Fluid

Phase separation in fluid additive hard sphere mixtures?

1998 ◽  
Vol 95 (2) ◽  
pp. 131-135 ◽  
Author(s):  
DOUGLAS HENDERSON DEZSO BODA KWONG-YU CHAN
Keyword(s):  
Phase Separation ◽  
Hard Sphere

Hard-sphere radii for the generalized Lindemann criterion

1998 ◽  
Vol 77 (5) ◽  
pp. 1441-1447
Author(s):  
S. Rabinovich, E. Brook-Levinson, E. Z
Keyword(s):  
Hard Sphere ◽  
Lindemann Criterion
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