Three body forces in the lattice dynamics of FCC metals
There are presently experimental data on FCC metals, concerning fundamentally harmonic properties (dispersion curves, second order elastic constants) and essentially anharmonic ones (third order elastic constants, thermal expansion). However, at present, there is not a simple interatomic potential t...
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todo:paper_00978485_v16_n4_p303_Barrera2023-10-03T14:56:50Z Three body forces in the lattice dynamics of FCC metals Barrera, G.D. Batana, A. There are presently experimental data on FCC metals, concerning fundamentally harmonic properties (dispersion curves, second order elastic constants) and essentially anharmonic ones (third order elastic constants, thermal expansion). However, at present, there is not a simple interatomic potential that can reproduce adequately all this experimental information simultaneously. In this work we develop several programs to calculate the second order elastic constants and the dispersion curves using a general central two body interaction up to 19th neighbors and common nearest neighbor three body interactions. The difference from previous works is that here the three body potential is a purely angular one, uncoupled from the two body forces, allowing a quantitative evaluation of its relative importance. © 1992. Fil:Barrera, G.D. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. Fil:Batana, A. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. JOUR info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/2.5/ar http://hdl.handle.net/20.500.12110/paper_00978485_v16_n4_p303_Barrera |
institution |
Universidad de Buenos Aires |
institution_str |
I-28 |
repository_str |
R-134 |
collection |
Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA) |
description |
There are presently experimental data on FCC metals, concerning fundamentally harmonic properties (dispersion curves, second order elastic constants) and essentially anharmonic ones (third order elastic constants, thermal expansion). However, at present, there is not a simple interatomic potential that can reproduce adequately all this experimental information simultaneously. In this work we develop several programs to calculate the second order elastic constants and the dispersion curves using a general central two body interaction up to 19th neighbors and common nearest neighbor three body interactions. The difference from previous works is that here the three body potential is a purely angular one, uncoupled from the two body forces, allowing a quantitative evaluation of its relative importance. © 1992. |
format |
JOUR |
author |
Barrera, G.D. Batana, A. |
spellingShingle |
Barrera, G.D. Batana, A. Three body forces in the lattice dynamics of FCC metals |
author_facet |
Barrera, G.D. Batana, A. |
author_sort |
Barrera, G.D. |
title |
Three body forces in the lattice dynamics of FCC metals |
title_short |
Three body forces in the lattice dynamics of FCC metals |
title_full |
Three body forces in the lattice dynamics of FCC metals |
title_fullStr |
Three body forces in the lattice dynamics of FCC metals |
title_full_unstemmed |
Three body forces in the lattice dynamics of FCC metals |
title_sort |
three body forces in the lattice dynamics of fcc metals |
url |
http://hdl.handle.net/20.500.12110/paper_00978485_v16_n4_p303_Barrera |
work_keys_str_mv |
AT barreragd threebodyforcesinthelatticedynamicsoffccmetals AT batanaa threebodyforcesinthelatticedynamicsoffccmetals |
_version_ |
1807320903423361024 |