Recently, a dislocation-free deformation mechanism was proposed by Kiritani
et al. on the basis of a series of experiments where thin foils of fee met
als were deformed at very high strain rates. In the experimental study, the
y observed a large density of stacking fault tetrahedra but very low disloc
ation densities in the foils after deformation. This was interpreted as evi
dence for a new dislocation-free deformation mechanism, resulting in a very
high vacancy production rate. In this paper we investigate this propositio
n using large-scale computer simulations of bulk and thin films of copper.
To favour such a dislocation-free deformation mechanism, we have made dislo
cation nucleation very difficult by not introducing any potential dislocati
on sources in the initial configuration. Nevertheless, we observe the nucle
ation of dislocation loops, and the deformation is carried by dislocations.
The dislocations are nucleated as single Shockley partials. The large stre
sses required before dislocations are nucleated result in a very high dislo
cation density, and therefore in many inelastic interactions between the di
slocations. These interactions create vacancies and a very large vacancy co
ncentration is quickly reached.