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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Detalles Bibliográficos
Autor principal: Barrera, G.D
Otros Autores: Batana, A.
Formato: Capítulo de libro
Lenguaje:Inglés
Publicado: 1992
Acceso en línea:Registro en Scopus
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Registro en la Biblioteca Digital
Aporte de:Registro referencial: Solicitar el recurso aquí
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100 1 |a Barrera, G.D. 
245 1 0 |a Three body forces in the lattice dynamics of FCC metals 
260 |c 1992 
270 1 0 |m Barrera, G.D.; Universidad de Buenos Aires, Facultad de Ciencias Exactas y Naturales, Departamento Química Inorgánica, Analítica y Química Física, Pab. 2, Ciudad Universitaria, 1428 Buenos Aires, Argentina 
506 |2 openaire  |e Política editorial 
504 |a Animalu, (1973) Phys. Rev., 8 B (8), p. 3555 
504 |a Bertoni, Bortolani, Calandra, Nizzoli, Third order perturbation theory and lattice dynamics of simple metals (1973) Journal of Physics F: Metal Physics, 4, p. 19 
504 |a Bertoni, Bisi, Calandra, Nizzoli, (1975) J. Phys. F, 5, p. 419 
504 |a Cousins, (1973) J. Phys. F, 3, p. 1915 
504 |a Liebfried, Ludwig, (1965) Solid St. Phys., 12, p. 275 
504 |a Lynn, Smith, Nicklow, (1973) Phys. Rev., 8 B, p. 3493 
504 |a Prakash, Upadhyaya, (1988) J. Phys. Chem. Solids, 49, p. 91 
504 |a Press, Flannery, Teulkosky, Vettering, (1986) Numerical Recipes, , Cambridge University Press, England 
504 |a Sarkar, Sengupta, Three body interaction in ionic crystals (1969) Solid State Communications, 7, p. 135 
504 |a Sharma, Upadhayaya, (1977) J. Phys. Chem. Solids, 38, p. 601 
504 |a Upadhyaya, Sharma, (1976) Phys. Rev., 14 B, p. 2692 
520 3 |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.  |l eng 
593 |a Universidad de Buenos Aires, Facultad de Ciencias Exactas y Naturales, Departamento Química Inorgánica, Analítica y Química Física, Pab. 2, Ciudad Universitaria, 1428 Buenos Aires, Argentina 
700 1 |a Batana, A. 
773 0 |d 1992  |g v. 16  |h pp. 303-310  |k n. 4  |p Comput. Chem.  |x 00978485  |w (AR-BaUEN)CENRE-1040  |t Computers and Chemistry 
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856 4 0 |u https://hdl.handle.net/20.500.12110/paper_00978485_v16_n4_p303_Barrera  |y Handle 
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