Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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-