Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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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)