Sodium clusters have a strong, collective resonance near 3 eV,
which (due to its large oscillator strength) can be multiply
excited by a relatively weak fs-laser pulse (109 to
1010W/cm2) [1]. The kinetic energy distribution of the
electrons emitted from such highly excited clusters is purely
Boltzmann-like, with a mean energy of about 1 eV. A model which can
explain all experimental data is as follows: The laser field
couples strongly to the collective motion of the nearly free
electron gas in the cluster. The interaction between collective and
single particle excitation (time constant about 10 fs) leads to an
effective electron temperature of 6000 to 8000K during the laser
pulse. The electronic energy flows with a time constant of about
one ps into ionic vibrations. Electrons are emitted, as long as the
electron gas is hot enough. The cluster cools further by
evaporation of atoms, which can finally lead to Coulomb assisted
break up.
[1] R.Schlipper, R.Kusche, B.v.Issendorff, H.Haberland, PRL 80, 1194
(1998)