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Aca - Departamento de Física - Universidad Técnica Federico Santa ...

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V Encuentro Sud Americano <strong>de</strong> Colisiones Inelásticas en la Materia<br />

Atomistic simulations of swift ion bombardment<br />

Eduardo M. Bringa 1<br />

1 CONICET & Instituto <strong>de</strong> Ciencias Básicas, <strong>Universidad</strong> Nacional <strong>de</strong> Cuyo, Mendoza 5500, Argentina<br />

email address corresponding author: ebringa@yahoo.com<br />

Atomistic simulations are often used<br />

to study the bombardment of ions in the regime<br />

where elastic collisions dominate, but<br />

they rarely mo<strong>de</strong>l bombardment when electronic<br />

effects dominate energy <strong>de</strong>position in<br />

the target. There are several mo<strong>de</strong>ls to inclu<strong>de</strong><br />

these electronic effects within classic<br />

molecular dynamics (MD) simulations like<br />

Coulomb explosions, “thermal spikes”, and<br />

etcetera. MD simulations follow the evolution<br />

of a system of atoms interacting trough<br />

some empirical potential. Using current parallel<br />

computers millions of atoms can be<br />

followed during tens of picoseconds. Such<br />

systems are large enough and can be studied<br />

long enough to account for the early stages<br />

of radiation damage. Later stages have to be<br />

studied with other techniques, like kinetic<br />

Monte Carlo or rate theory.<br />

Ion tracks [1], surface craters [2] or<br />

hillocks, electronic sputtering [3], and other<br />

radiation damage indicators can be predicted<br />

in this way. Examples from materials<br />

science, surface physics, and astrophysics<br />

will be shown to illustrate that these mo<strong>de</strong>ls<br />

are relatively simple, but provi<strong>de</strong> a reasonable<br />

<strong>de</strong>scription of experimental results when<br />

electronic stopping power cannot be neglected.<br />

Future directions to <strong>de</strong>scribe electronic<br />

effects in atomistic simulations will<br />

also be discussed.<br />

This work has been carried out in<br />

collaboration with several people, including<br />

D. Schwen, D. Farkas, J. Monk, A.<br />

Caro, J. Rodriguez-Nieva, T. Cassidy,<br />

R.E. Johnson, R. Papaléo, M. Da Silva, C.<br />

Ruestes, and Nestor Arista.<br />

Figure 1. MD simulation of hillocks in tetrahedral<br />

amorphous carbon, showing increasing hillock<br />

height with increasing electronic stopping [4].<br />

References<br />

[1] R. Devanathana, P. Durhamb, J. Dua, L.R.<br />

Corrales and E.M. Bringa, Nuclear Instruments<br />

and Methods in Physics Research Section B 255,<br />

172 (2007).<br />

[2] E.M. Bringa, R.E. Johnson, R. M. Papaléo,<br />

Phys. Rev. B 65, 094113 (2002).<br />

[3] E.M. Bringa and R.E. Johnson, Phys. Rev.<br />

Lett. 88, 165501 (2002).<br />

[4] D. Schwen and E.M. Bringa, submitted<br />

(2010).<br />

18 Valparaíso, Chile

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