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Physik: DPG Tagungen - Sitzung O 28 - Nano-science.de

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<strong>Physik</strong>: <strong>DPG</strong> <strong>Tagungen</strong> - <strong>Sitzung</strong> O <strong>28</strong><br />

http://www.dpg-tagungen.<strong>de</strong>/archive/2004/o_<strong>28</strong>.html<br />

Bildkontrast empfindlich von <strong>de</strong>r ausgewählten Energie <strong>de</strong>r Elektronen abhängt. Die <strong>de</strong>rzeitige Begrenzung <strong>de</strong>r<br />

räumlichen (160nm) und zeitlichen Auflösung <strong>de</strong>r Metho<strong>de</strong> ist durch die Repetitionsrate (1kHz) <strong>de</strong>s anregen<strong>de</strong>n<br />

Lasers bedingt.<br />

O <strong>28</strong>.35 Poster Mi 16:00 Bereich C<br />

Growth of Platin <strong>Nano</strong>wire Networks on Nafion<br />

•M. Elbahri, J. Franc, O.C. Aktas, R. A<strong>de</strong>lung und F. Faupel<br />

Lehrstuhl für Materialverbun<strong>de</strong>, Technische Fakultät <strong>de</strong>r CAU Kiel<br />

The Nafion polymer, produced by the Dupont company, is still the most prominent membrane material for the<br />

commercial polymer electrolyte fuel cell (PMFC). Usually, the Nafion membrane is sandwiched by two catalytic<br />

layers, consisting of a metal-Nafion-carbon mixture in or<strong>de</strong>r to provi<strong>de</strong> catalytic activity as well as electrical and<br />

proton conductivity. It turns out that most of the Platinum doesn't contribute to the catalytic efficiency, which<br />

increases the total cost for the PMFC-fuel cell. An alternative approach might be a catalytic layer formed by a<br />

Pt-nanowire network. We present here a strategy to <strong>de</strong>posit Pt in the form of a nanowire networks. Therefore<br />

we used sputter <strong>de</strong>posited Pt on a vacuum <strong>de</strong>posited amorphous carbon mask layer. We show different<br />

Pt-nanowire networks generated on the Nafion surface and discuss the mechanisms that tune the network<br />

parameters like nanowire dimensions and mesh width.<br />

The authors thank the Technologiestiftung Schleswig-Holstein for supporting the project.<br />

O <strong>28</strong>.36 Poster Mi 16:00 Bereich C<br />

Imaging of optical near fields of nanostructures with fs laser pulses<br />

•Juliane Birk, Johannes Boneberg und Paul Lei<strong>de</strong>rer<br />

Universität Konstanz, FB <strong>Physik</strong>, LS Lei<strong>de</strong>rer, SFB 513, 78457 Konstanz<br />

The optical properties of nanostructures are a topic of interesting investigations. In analogy to the near fields<br />

around a Hertz dipole we expect near fields in the surrounding of all nanostructures. Up to now they were<br />

analysed with the scanning near field optical microscope (SNOM). We want to introduce an alternative method<br />

to image near fields with intensive short laser pulses. The intensity is adjusted to values where the substrate far<br />

from the particle is not affected. Nevertheless, the surface around and below the particle can be ablated, due to<br />

the local intensity enhancement in the optical near field. After the laser pulse the modified surface is imaged with<br />

atomic force microscopy (AFM) and thus the optical near fields of different nanostructures on several<br />

substrates, for example silicon, can be studied. A few examples of the near fields of various nanostructures are<br />

shown.<br />

O <strong>28</strong>.37 Poster Mi 16:00 Bereich C<br />

Infrared-optical properties of Cu nanoparticles on CaF 2 (111)<br />

•Birgit Gehring, Andreas Priebe und Annemarie Pucci<br />

Kirchhoff-Institut für <strong>Physik</strong>, Im Neuenheimer Feld 227, D - 69120 Hei<strong>de</strong>lberg<br />

Using IR spectroscopy the growth of Cu nanoparticles on UHV-cleaved CaF 2 (111) was investigated in situ.<br />

Relative transmission spectra informed about the dynamic conductivity of the nanoparticle film and about the<br />

influence of the substrate temperature on the percolation threshold.<br />

In the range from about 1000 cm -1 up to about 2500 cm -1 a relative transmission > 100 % was observed for Cu<br />

coverage below percolation, which corresponds to an anti-reflection effect. The magnitu<strong>de</strong> of this effect<br />

<strong>de</strong>pends on the growth temperature.<br />

For certain average Cu thicknesses we exposed CO at a sample temperature of about 100 K. The CO adsorption<br />

on different Cu facets was studied by IR transmission spectroscopy. The morphology of the nanoparticle layer<br />

13 of 32 07.06.2009 22:14

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