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Plenarvorträge - DPG-Tagungen

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Dynamik und Statistische Physik Dienstag<br />

DY 27 Quantum Chaos<br />

Zeit: Dienstag 16:30–18:15 Raum: H3<br />

DY 27.1 Di 16:30 H3<br />

Microwave measurements on dielectric quadrupole billards —<br />

•R. Schäfer and H.-J. Stöckmann — Fachbereich Physik, Philipps-<br />

Universität Marburg, Renthof 5, D-35032 Marburg, Germany<br />

Quadrupole dielectic billiards have received a lot of attention because<br />

of their highly directed emission patterns [1] which is a welcome effect in<br />

the design of microdisc lasers. We measured transmission spectra from a<br />

fixed antenna inside the disc to a moveable antenna, thus scanning both<br />

the inside and outside region of the teflon disc. A Fourier transform of<br />

the spectra yields the pulse propagation. The long time behavior is dominated<br />

by the whispering gallery modes, which decay very slowly due to<br />

total internal reflection. The emission pattern of the quadrupole billiard<br />

is strongly influenced by the structures of its mixed phase space. Even for<br />

strong deformations with no stable islands left, a high directionality of<br />

the emission is found. This can be explained by the unstable manifolds of<br />

periodic orbits [2]. The internal dynamics of the pulse has been analyzed<br />

by means of Husimi distributions, while for the outer region the Poynting<br />

vector was calculated to obtain the emission pattern. Both are compared<br />

with classical ray dynamics taking into account the curvature-corrected<br />

Fresnel formula.<br />

[1] J.U. Nöckel, A.D. Stone, Nature 385, 45 (1997)<br />

[2] H.G.L Schwefel et al., arXiv:physics/0308001<br />

DY 27.2 Di 16:45 H3<br />

Quantum Chaos on Networks — •Holger Schanz — Max-Planck<br />

Institut für Strömungsforschung und Institut für Nichtlineare Dynamik<br />

der Universität Göttingen, Bunsenstr. 10, 37073 Göttingen<br />

Quantized networks are simple models which allow to study quantum<br />

signatures of classical chaos. They allow analytical approaches to unsolved<br />

problems in quantum chaos, including periodic-orbit theories for<br />

spectral correlations, transport and localization phenomena as well as<br />

scarring of wavefunctions. A brief account of the model and the obtained<br />

results will be given.<br />

H. Schanz and U. Smilansky, Phys. Rev. Lett. 84(00)1427.<br />

G. Berkolaiko, H. Schanz, R. S. Whitney, Phys. Rev. Lett. 88(02)104101.<br />

H. Schanz and T. Kottos, Phys. Rev. Lett. 90(03)234101.<br />

H. Schanz, M. Puhlmann and T. Geisel, Phys. Rev. Lett. 91(03)134101.<br />

DY 27.3 Di 17:00 H3<br />

Ray-wave correspondence in a fully chaotic quasi-stadium laser<br />

resonator — •J. Wiersig 1 , T. Fukushima 2 , and T. Harayama 3<br />

— 1 Universität Bremen — 2 Okayama Prefectural University, Okayama,<br />

Japan — 3 ATR Adaptive Communication Research Laboratories, Kyoto,<br />

Japan<br />

The relation between resonator modes and unstable periodic orbits in<br />

a fully chaotic quasi-stadium laser resonator is investigated. The complicated<br />

wavelength dependence of the power coupling coefficient is explained<br />

by a simple coupling model, which considers some unstable periodic<br />

orbits.<br />

DY 27.4 Di 17:15 H3<br />

Semiclassical approximations for open systems: transport and<br />

decay — •Mathias Puhlmann, Holger Schanz, Tsampikos Kottos,<br />

and Theo Geisel — Max-Planck Institut für Strömungsforschung<br />

und Institut für Nichtlineare Dynamik der Universität Göttingen, Bunsenstr.<br />

10, 37073 Göttingen<br />

DY 28 Glasses I (joint session DF/DY)<br />

Important and diverse physical applications like electronic transport<br />

through mesoscopic devices or microcrystal lasers require an understanding<br />

of open quantum systems with chaotic classical limit. For many interesting<br />

processes in such systems the interference between classical trajectories<br />

is decisive. Therefore the standard semiclassical theory based on<br />

the diagonal approximation is not accurate or fails at all. Using quantum<br />

graphs as model systems we show how one can improve the semiclassical<br />

description such that shot noise and the short-time devitions from a<br />

simple exponential probability decay are reproduced.<br />

H. Schanz, M. Puhlmann and T. Geisel, Phys. Rev. Lett. 91(03)134101.<br />

DY 27.5 Di 17:30 H3<br />

Semiclassical approach to shot noise in chaotic systems —<br />

•Andreas Lassl, Marko Turek, and Klaus Richter — Institut<br />

für Theoretische Physik, Universität Regensburg, D-93040 Regensburg<br />

We propose a semiclassical approach to shot noise in clean chaotic<br />

systems [1]. Starting from the semiclassical expression for the transmission<br />

we derive the Fano factor in terms of classical paths. As expected<br />

the application of the diagonal approximation yields a vanishing result<br />

for the Fano factor. Therefore one has to include action correlations between<br />

classical paths which can be expressed in terms of a crossing angle<br />

distribution as in [2]. Here we present detailed numerical studies of this<br />

crossing angle distribution in open systems.<br />

[1] C.W.J. Beenakker and C. Schönenberger, Physics Today, 56 (5), 37-<br />

42 (2003)<br />

[2] K. Richter and M. Sieber, PRL 89, 206801 (2002)<br />

DY 27.6 Di 17:45 H3<br />

Universal spectral form factor for chaotic dynamics I: The<br />

Hadamard-Gutzwiller model — Stefan Heusler, •Sebastian<br />

Müller, Petr Braun, and Fritz Haake — Fachbereich Physik, Universität<br />

Duisburg-Essen, 45117 Essen<br />

We consider the semiclassical limit of the spectral form factor K(τ) of<br />

the Hadamard-Gutzwiller model. Starting from the Gutzwiller type double<br />

sum over classical periodic orbits we set out to recover the universal<br />

behavior predicted by random-matrix theory, both for dynamics with and<br />

without time reversal invariance. For times smaller than half the Heisenberg<br />

time TH ∝ ¯h −f+1 , we extend the previously known τ-expansion to<br />

include the cubic term. Our results exemplify the “diagrammatic rules”<br />

determining the families of orbit pairs responsible for all orders of the<br />

τ-expansion.<br />

DY 27.7 Di 18:00 H3<br />

Universal spectral form factor for chaotic dynamics II: General<br />

systems — •Stefan Heusler, Sebastian Müller, Petr Braun<br />

und Fritz Haake — Fachbereich Physik, Universität Duisburg-Essen,<br />

45117 Essen<br />

We consider the semiclassical limit of the spectral form factor K(τ)<br />

of general, fully hyperbolic dynamics. Generalizing results for the<br />

Hadamard-Gutzwiller model, we discuss the families of orbit pairs giving<br />

rise to higher-order contributions to the spectral form factor.<br />

Zeit: Dienstag 09:30–12:30 Raum: H23<br />

Hauptvortrag DY 28.1 Di 09:30 H23<br />

Theory of the glass transition for systems with trivial statics —<br />

•Rolf Schilling 1 and Grzegorz Szamel 2 — 1 Institut für Physik,<br />

Johannes Gutenberg-Universität, D-55099 Mainz — 2 Department of<br />

Chemistry, Colorado State University, Ft. Collins, CO 80523, USA<br />

The mode coupling theory (MCT) derived and investigated in great<br />

detail by Götze and his coworkers has been the most important step to-<br />

wards the microscopic understanding of the structural glass transition.<br />

MCT yields a glass transition if the static correlations reach a critical<br />

value. However, there exist systems with trivial statics where static correlations<br />

even vanish. Nevertheless they exhibit a discontinuous glass<br />

transition which can not be described by MCT in its present form. In<br />

a first step we have derived a self-consistent equation for the diffusion<br />

constant which yields a continuous transition, in contrast to simulational

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