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Plenarvorträge - DPG-Tagungen

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Chemische Physik und Polymerphysik Montag<br />

W. Nadler, P. Grassberger, J. Chem. Phys. 118 (2002) 444.<br />

[2] T. Prellberg, A.L. Owczarek, Phys. Rev. E 62 (2000) 3780.<br />

CPP 5.5 Mo 11:00 H 39<br />

Time-depedent density functional theory applied in molecules,<br />

liquids and solids — •Ari P Seitsonen and Jürg Hutter — Universität<br />

Zürich<br />

Time-dependent density functional theory (TDDFT) is a versatile<br />

method which can be applied also to the determination of excitation<br />

CPP 6 Self-organising Systems<br />

energies in materials similarly as the density functional theory (DFT)<br />

in the ground state. We apply the new implementation [J. Hutter, JCP<br />

(2003)] of the method in the CPMD code. This enables us to calculate<br />

the excitation energies and properties such as forces on the ions in the excited<br />

state, employing the plane wave basis set/pseudo potential method.<br />

We report applications in molecules, liquids and solids, and we discuss<br />

both the advantages and the shortcomings of the method. As examples<br />

we mention small molecules, solvation of tetrazine and acetone in water<br />

and defects in diamond.<br />

Zeit: Montag 11:30–12:15 Raum: H 39<br />

CPP 6.1 Mo 11:30 H 39<br />

Combinatorial mapping of PS-b-P2VP-b-PtBMA triblock<br />

copolymers in thin films — •S. Ludwigs 1 , K. Schmidt 1 , R.<br />

Magerle 1 , G. Krausch 1 , C. Stafford 2 , M. Fasolka 2 , A. Karim 2 ,<br />

E. Amis 2 , A. Zvelindovsky 3 , and A. Sevink 3 — 1 Physikalische<br />

Chemie II, Universität Bayreuth, Bayreuth, Germany — 2 NIST<br />

Combinatorial Methods Group, Gaithersburg, USA — 3 Leiden Institute<br />

of Chemistry, Leiden, Netherlands<br />

Using sequential living anionic polymerization we synthesized a series<br />

of monodisperse PS-b-P2VP-b-PtBMA triblock copolymers (SVT)with<br />

increasing molecular weight of the poly(tert butyl methacrylate) block 1 .<br />

In the present contribution we show experimental results on the thin<br />

film behavior of SVT with volume fractions φPS : φP2V P : φPtBMA =<br />

1 : 1.2 : x (with x ranging from 3.05 to 4). Gradients in film thickness<br />

were prepared via thin film flow coating of dilute solutions in chloroform.<br />

On controlled annealing in a non-selective solvent the films form<br />

terraces of well-defined thickness exhibiting a highly ordered perforated<br />

lamellar structure. With an additional gradient in substrate surface energy<br />

orthogonal to the gradually increasing film thickness we find that<br />

the perforated lamellar phase is formed irrespective of the chemical nature<br />

of the substrate which makes the structure useful for applications in<br />

nanotechnology 2 . We support our experimental results with simulations<br />

based on the dynamic density functional theory: with increasing size of<br />

the simulation box we find a similar sequence of structures as in the experiments.<br />

1 S. Ludwigs et al., Polymer 44, 6815 (2003). 2 S. Ludwigs et<br />

al., Nature Materials 2, 744 (2003).<br />

CPP 6.2 Mo 11:45 H 39<br />

AFM CHARACTERIZATION OF SUPPORTED PHOSPHO-<br />

LIPID LAYERS FORMED BY SOLUTION SPREADING —<br />

•T. Spangenberg 1 , N.F. de Mello 2 , T.B. Creczynski-Pasa 3 ,<br />

A.A. Pasa 4 , and H. Niehus 1 — 1 Humboldt-Universität zu Berlin, Institut<br />

für Physik, Newtonstr. 15, 12489 Berlin — 2 Pós-graduação em<br />

Química, Universidade Federal de Santa Catarina, Florianópolis, Brazil<br />

— 3 Departamento de Ciências Farmacêuticas, Universidade Federal de<br />

Santa Catarina, Florianópolis, Brazil — 4 Departamento de Física, Universidade<br />

Federal de Santa Catarina, Florianópolis, Brazil<br />

CPP 7 Physics of Polymers I<br />

The morphology and the stability of supported phospholipid (DPPC,<br />

DOPC) layers prepared by solution spreading on mica were investigated<br />

by atomic force microscopy. The samples were analyzed after the solvent<br />

evaporation, the hydration step and after immersion in a buffer solution.<br />

The phospholipid layers prepared by solution spreading method were successfully<br />

characterized by ex-situ and in-situ AFM measurements. This<br />

sequence of measurements allows us to follow the surface rearrangement<br />

of the lipidic material, from non-uniform deposits, through multilayer<br />

structures, to a final pattern with large bilipidic terraces. The most significant<br />

result was the imaging of the prepared phospholipid layers in-situ<br />

after the immersion in the liquid cell. The systems investigated exhibited<br />

a stable surface configuration during the measurements, which is suitable<br />

for studying time dependent biological and physical phenomena.<br />

CPP 6.3 Mo 12:00 H 39<br />

Chemically driven running drops — •Uwe Thiele, Karin John,<br />

and Markus Bär — Max-Planck Institut für Physik komplexer Systeme,<br />

Nöthnitzer Str.38, 01138 Dresden<br />

A continuous dynamic model for the movement of a drop on a solid<br />

substrate is derived for (1) driving by an externally given gradient using<br />

a wettability gradient as an example and (2) driving by a self-produced<br />

wettability gradient. The latter case of self-propelled drops on reactive<br />

substrates corresponds to such experimentally found free-running<br />

droplets (Dos Santos, D. F. and Ondarcuhu, T., PRL 75, 2972 (1995)).<br />

The moving-droplet solutions of the model are investigated in detail.<br />

Zeit: Montag 14:00–15:30 Raum: H 37<br />

CPP 7.1 Mo 14:00 H 37<br />

Scaling properties of critical polymer blends and polymer solutions<br />

near the glass transition — •Werner Köhler, Wolfgang<br />

Enge, and Jürgen Rauch — Physikalisches Institut, Universität<br />

Bayreuth, 95440 Bayreuth<br />

Critical polymer blends show Ising-like critical scaling close to Tc and<br />

mean-field behavior for larger ǫ = (T − Tc)/Tc. Because of the thermal<br />

activation of the Onsager coefficient, however, the critical exponent γ cannot<br />

be directly observed in the temperature dependence of the diffusion<br />

coefficient D within the mean-field regime. Similarly, the diffusion coefficient<br />

of semidilute and concentrated polymer solutions typically only approaches<br />

the concentration scaling law but then rapidly decreases because<br />

of the increasing glass temperature of the solution. Contrary to D, the<br />

Soret coefficient ST is neither sensitive to thermal activation of the Onsager<br />

coefficient nor to the increase of local friction at the glass transition<br />

and shows clean scaling in both cases. Experiments have been performed<br />

on semidilute and concentrated solutions of polystyrene in toluene and<br />

on critical poly(dimethylsiloxane)/poly(ethyl-methylsiloxane) mixtures.<br />

CPP 7.2 Mo 14:15 H 37<br />

Surface glass transition of monodisperse polystyrenes and<br />

their bimodal mixtures investigated by the embedding of<br />

noble metal nanoclusters and the XPS-charging effect —<br />

•Jörn Erichsen, Tesfaye Shiferaw, Jörn Kanzow, Ulrich<br />

Schürmann, Vladimir Zaporojtchenko, and Franz Faupel —<br />

Lehrstuhl für Materialverbunde, Faculty of Engineering,<br />

The temperature dependent embedding process of noble metal nanoclusters<br />

into polymers was used to probe the surface glass transition.<br />

X-ray photoelectron spectroscopy (XPS) was applied to study the embedding<br />

of Au nanoclusters into polystyrene [1]. Previously a small decrease<br />

of glass transition temperature (Tg) at the surface compared to the bulk,<br />

which decreases at low Mw, was detected with this method [1]. The Tg of<br />

thin PS films was additionally determined by the charging and discharg-

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