09.12.2012 Views

Plenarvorträge - DPG-Tagungen

Plenarvorträge - DPG-Tagungen

Plenarvorträge - DPG-Tagungen

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

Dynamik und Statistische Physik Dienstag<br />

DY 25.5 Di 16:00 H3<br />

Fast Crack Growth by Surface Diffusion — •Robert Spatschek<br />

and Efim Brener — Institut für Festkörperforschung, Forschungszentrum<br />

Jülich, 52425 Jülich<br />

Fracture is an intriguing irreversible phenomenon that plays an important<br />

role in our day-to-day-life. Crack propagation is responsible for the<br />

vast field of material failure but is also an interesting subject of physical<br />

research. In particular, it exhibits several peculiarities for higher propagation<br />

velocities. Here we present a continuum theory which describes<br />

the fast growth of a crack by surface diffusion. By introducing a fully<br />

dynamical theory of elasticity, it is possible to obtain a self-consistent<br />

selection of the crack tip radius. This theory describes the complicated<br />

dynamics of a crack tip, the saturation of the steady state velocity appreciably<br />

below the Rayleigh speed, and the blunting of the crack tip.<br />

Furthermore, it includes the possibility of a tip splitting instability for<br />

high applied tensions.<br />

DY 25.6 Di 16:15 H3<br />

Stabilität hexagonaler Erstarrungsmuster — •Mathis Plapp —<br />

Laboratoire de Physique de la Matière Condensée, Ecole Polytechnique,<br />

91128 Palaiseau, Frankreich<br />

DY 26 General Statistical Physics<br />

Hexagonale Muster bilden sich in vielen Nichtgleichgewichtssituationen,<br />

wenn eine zweidimensionale Translationinvarianz durch eine dynamische<br />

Instabilität gebrochen wird. Bei der gerichteten Erstarrung von<br />

Legierungen bilden sich oberhalb einer kritischen Erstarrungsgeschwindigkeit<br />

zelluläre Strukturen, die sich im dreidimensionalen Fall zu hexagonalen<br />

Mustern ordnen. In Dünnschichtexperimenten und numerischen<br />

Arbeiten wurde gezeigt, dass die Stabilität solcher Erstarrungszellen in<br />

zwei Dimensionen erheblich von der Anisotropie der Grenzfläche abhängt.<br />

Hier wird nun mittels Phasenfeld-Simulationen der dreidimensionale Fall<br />

untersucht. Die räumliche Struktur der Instabilitätsmoden wird von der<br />

Symmetrie des Zellenmusters bestimmt; die Stabilitätsgrenzen hängen<br />

stark von der Anisotropie ab. Quadrat- und Streifenmuster sind unstabil.<br />

Ausser Sechsecken wurde ein weiteres stabiles Muster gefunden: Tripletts,<br />

die aus drei assymmetrischen Zellen bestehen. Sie lassen sich durch<br />

zeitlich begrenzte Störungen kontrolliert aus Sechsecken erzeugen.<br />

Zeit: Dienstag 16:45–18:00 Raum: H2<br />

DY 26.1 Di 16:45 H2<br />

Long-term correlations distinguish coarsening mechanisms<br />

in alloys — •Lorenz-M. Stadler 1 , Bogdan Sepiol 1 , Richard<br />

Weinkamer 2 , Markus Hartmann 2 , Peter Fratzl 2 , Jan W.<br />

Kantelhardt 3 , Federico Zontone 4 , Gerhard Grübel 4 , and<br />

Gero Vogl 1 — 1 Institut für Materialphysik, Universität Wien, 1090<br />

Wien, Austria — 2 Max-Planck-Institute of Colloids and Interfaces,<br />

Department of Biophysics, 14424 Potsdam, Germany — 3 Institut<br />

für Theoretische Physik III, Justus-Liebig-Universität Giessen, 35392<br />

Giessen, Germany — 4 ESRF, BP 220, 38043 Grenoble Cedex, France<br />

We determine long-term correlations in the time series of fluctuating<br />

x-ray speckle intensities. A fluctuation analysis of small angle x-ray<br />

scattering data of the two phase-separating alloys Al-6at.%Ag and Al-<br />

9at.%Zn at late stages of phase separation reveals long-term correlations<br />

that are dramatically different for the two systems. From a comparison<br />

with recent Monte Carlo simulations we conclude that two different coarsening<br />

mechanisms are predominant in the two alloys—coarsening either<br />

by diffusion of single atoms or by movement of whole precipitates.<br />

We acknowledge financial support from the Austrian Federal Ministry<br />

for Education, Science and Culture (project GZ 45.529/2-VI/B/7a/2002)<br />

and the Hahn-Meitner-Institute Berlin in cooperation with the University<br />

of Potsdam.<br />

DY 26.2 Di 17:00 H2<br />

Domain-Wall Energy Analysis of exact Ground States for<br />

±J SG model in D=2 — •Amoruso Carlo and Alexander<br />

K.Hartmann — Institute for Theoretical Physics, Göttingen<br />

Computing ground states of Spin Glasses is a NP-hard problem, this<br />

means that only algorithms are known, where the running time in the<br />

worst case increases exponentially with the system size. For the special<br />

case of two-dimensional spin glasses without an external field and with<br />

periodic boundary conditions in at most one direction, efficient polynomial<br />

algorithms for the calculation of exact ground states are available.<br />

By using a matching algorithm, we computed exact ground states of two<br />

dimensional Ising Spin Glasses with a certain concentration of antiferromagnetic<br />

bonds p up to size L = 700. We calculated with high precision<br />

the critical concentration of pc at which the ferromagnetic phase ceases to<br />

exist, obtaining pc = 0.103(1). If the Nishimori point pN is located on the<br />

phase boundary (as believed), the phase diagram has a small reentrance,<br />

since pN ∼ 0.110. Besides we show that there is no spin-glass phase at<br />

finite temperature.<br />

DY 26.3 Di 17:15 H2<br />

Ground-state structure of the vertex-cover problem —<br />

•Wolfgang Barthel and Alexander K. Hartmann — Institute<br />

for Theoretical Physics, Göttingen<br />

Hard combinatorical optimization problems play an important role in<br />

Theoretical Computer Science. One is especially interested in the time<br />

complexity of such problems, i.e. how fast a typical instance can be solved<br />

depending on its size. It is expected that this is strongly connected to<br />

the landscape of the ground state structure of this problems. Here we<br />

consider the vertex-cover problem: Take a random graph consisting of<br />

undirected edges that meet at vertices and put guards on the vertices<br />

such that there is one at at least one endpoint of every edge. Solutions<br />

are covers which need a minimal number of guards and usually there is<br />

an exponential number of them. We numerically analyze the landscape<br />

of the solution space. A change in the ground state structure is observed<br />

at the point where all known fast algorithms fail.<br />

DY 26.4 Di 17:30 H2<br />

High-Loop Variational Calculation of the Effective Potential —<br />

•Sebastian Brandt and Axel Pelster — Institut für Theoretische<br />

Physik, Freie Universität Berlin, Arnimallee 14, D-14195 Berlin, Germany<br />

The thermodynamic properties of a quantum mechanical point particle<br />

moving in a one-dimensional potential V (x) follow from its effective potential<br />

Veff(X) where X denotes the path average. For zero temperature<br />

we present an efficient high-loop calculation of Veff(X) based on algebraic<br />

recursion relations. In case of an anharmonic oscillator with x 3 and x 4<br />

interactions we resum the divergent loop expansion via variational perturbation<br />

theory. Using both frequency and position of a trial oscillator<br />

as variational parameters, we determine the ground-state energy of the<br />

above anharmonic oscillator for arbitrary coupling strength. For pure x 4<br />

interaction, we furthermore extend our approach to D spatial dimensions<br />

and investigate, in particular, the large D-limit.<br />

DY 26.5 Di 17:45 H2<br />

Three-phase contact line interface profiles in electric fields<br />

— •Juergen Buehrle, Stephan Herminghaus, and Frieder<br />

Mugele — University of Ulm; Applied Physics Department; D-89069<br />

Ulm<br />

Conductive or electrolytic liquid droplets in electric fields assume an<br />

apparent contact angle (the angle assumed by the droplet shape far away<br />

from the contact line) which is different from Young’s angle. This effect<br />

was investigated in detail and new quantitative expressions for the contact<br />

angle deviation are derived. In the vicinity of the contact line longrange<br />

electric fields deform the liquid interface profile. We have investigated<br />

the equilibrium profiles by balancing electrostatic and capillary<br />

forces locally at the liquid vapor interface. Numerical results suggest that<br />

the contact angle at the contact line is equal to Young’s angle. Simultaneously,<br />

the local curvature displays a weak algebraic divergence. We<br />

present an asymptotic analytical model, which confirms these results and<br />

elucidates the scaling behavior of the profile close to the contact line. (see<br />

also J. Buehrle, S. Herminghaus, and F. Mugele, Phys. Rev. Lett., 2003,<br />

91, 86101)

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!