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Generation of metal nanodroplets and impact experiments<br />
A. Habenicht ∗ ,P.Leiderer ∗ andJ.Boneberg ∗<br />
Flat metal nanostructures on inert substrates like glass, silicon or graphite are<br />
illuminated by single intensive laser pulses with fluences above the melting threshold.<br />
The liquid structures produced in this way are far from their equilibrium shape and<br />
a dewetting process sets in. On a timescale of a few nanesconds, the liquid contracts<br />
toward a sphere. During this contraction the center of mass moves upward, which can<br />
lead to detachment of droplets from the surface due to inertia. The velocity of the<br />
detaching nanodroplets is measured with a light barrier technique 1 .Theexperiment<br />
shows (see figure 1a) that the velocity of the detached droplet is constant over a<br />
large range of laser energy densities. This supports the model of a dewetting driven<br />
process: The droplet gains surface energy by contracting toward a sphere which is<br />
then converted into kinetic energy. Results are shown for different materials, where<br />
different surface tensions result in different velocities.<br />
Further we show impact experiments where the droplets are landed on another<br />
substrate. The particles cool down during the flight due to thermal radiation. They<br />
solidify either during flight or when impacting on the substrate. By catching the particles<br />
at different distances, the landing temperature can be varied. A droplet which<br />
is still molten at impact, spreads (and, under certain circumstances, even rebounds)<br />
until the heat loss into the substrates leads to solidification of the particle. Snapshots<br />
of different stages of droplet impact are shown (see figure 1b).<br />
∗ University of Konstanz, Dept. of Physics, LS Prof. Dr. Leiderer, D-78457 Konstanz, Germany.<br />
1 Habenicht et al., Science 309, 2043 (2005).<br />
Velocity (m/s)<br />
80<br />
60<br />
40<br />
20<br />
a) b)<br />
0<br />
0 1 2 3 4<br />
Laser energy density F/FC Figure 1: (a) Velocity of the detached gold particles as a function of the energy density<br />
of the melting laser. The velocity is constant of a large area of energy densities due<br />
to conversion of surface energy into kinetic energy (b) Impact of gold droplets with<br />
different sizes on silicon. Depending on the landing temperature (and thus the size of<br />
the particle) the droplets solidify at different stages (shown on the right) of droplet<br />
impact.<br />
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