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Abstracts - KTH Mechanics

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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 />

185

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