Monte Carlo and lattice-dynamics studies of the thermal and elastic properties of a rigid-ion model of sodium chloride

1988 ◽  
Vol 38 (15) ◽  
pp. 10820-10829 ◽  
Author(s):  
Zhaoxin Gong ◽  
G. K. Horton ◽  
E. R. Cowley
2016 ◽  
Vol 58 (3) ◽  
pp. 269-279 ◽  
Author(s):  
Hassan S. Hedia ◽  
Saad M. Aldousari ◽  
Ahmed K. Abdellatif ◽  
Gamal S. Abdelhaffez

1971 ◽  
Vol 9 (3) ◽  
pp. 185-189 ◽  
Author(s):  
K.V. Namjoshi ◽  
S.S. Mitra ◽  
J.F. Vetelino

2014 ◽  
Vol 490 ◽  
pp. 012059 ◽  
Author(s):  
A V Lugovskoy ◽  
M P Belov ◽  
Yu Kh Vekilov ◽  
O M Krasilnikov

1967 ◽  
Vol 20 (5) ◽  
pp. 495 ◽  
Author(s):  
J Oitmaa

The lattice dynamics of harmonic and anharmonic shell models are reviewed. It is shown that the various dynamical equations for the shell model can be expressed in the same form as those for the rigid ion model, but with modified force constants. The anharmonic shell model leads to higher order contributions to the dipole moment, quadratic and cubic in the normal coordinates, for which explicit expressions are obtained.


The electronic contribution to the dynamical tensors is examined in more detail and the following results are obtained. First the electronic contribution is shown to be translationally invariant, secondly the assumption that this term can be approximately represented by a two-body interaction is shown to be equivalent to a rigid ion model, and finally this approximation is shown to become exact in the limit q = 0.


2008 ◽  
Vol 147 (5-6) ◽  
pp. 221-225 ◽  
Author(s):  
Gökhan Gökoğlu ◽  
Aytaç Erkişi

2007 ◽  
Vol 21 (05) ◽  
pp. 249-259 ◽  
Author(s):  
K. BOUAMAMA ◽  
P. DJEMIA

Structural and elastic properties as well as lattice dynamics of ternary MgS x Se 1-x alloy have been studied using first-principles calculations. These are done using density functional theory (DFT) and density functional perturbation theory (DFPT) within the local density approximation (LDA) and employing the virtual-crystal approximation (VCA). We found that the lattice parameter, the elastic constants and the phonon frequencies follow a quadratic law in x.


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