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Tiefe Temperaturen Montag are composite spinon-phonon objects. Second, the change of the magnetization and the corresponding change of the wave vector of the spinons strongly affects the way in which various umklapp processes can relax the heat current, leading to a characteristic fractal-like spiky behavior of κ(T, h) as a function of h. [1] E. Shimshoni, N. Andrei and A. Rosch, Phys. Rev. B 68, 104401 (2003). TT 3.11 Mo 12:00 H18 ESR study of the low-dimensional quantum spin system TiOCl — •V. Kataev 1,2 , J. Baier 2 , A. Möller 3 , L. Jongen 3 , G. Meyer 3 und A. Freimuth 2 — 1 Leibniz-Institut für Festkörper- und Werkstoffforschung PF D-01171 Dresden — 2 II. Physikalisches Institut, Universität zu Köln, D-50937 Köln — 3 Institut für Anorganische Chemie, Universität zu Köln, D-50939 Köln We present electron spin resonance (ESR) measurements of Ti 3+ (3d 1 ) ions in single crystals of the novel layered quantum spin magnet TiOCl [1]. The ESR data give evidence that the single electron in the d-shell occupies predominantly the dxy orbital which lies in the bc crystallographic plane. This result suggests a formation of a spin-1/2 chain along the b direction, owing to the overlap of the orbital states, and supports recent LDA+U calculations of the band structure [2]. The ESR signal vanishes at Tc=67 K signalling the transition to a non-magnetic, possibly a spin- Peierls state, as proposed in Ref. [2]. Our x-ray powder diffraction data give however no evidence for the structural transition associated with the spin-gap transition. A pronounced dependence of the linewidth and the g factor on temperature suggests a strong coupling of spins to the lattice which may be decisive for the magnetic properties of TiOCl. In connection with the peculiar temperature dependence of the ESR parameters we discuss the role of spin and probably also orbital fluctuations above Tc for the opening of the spin gap. [1] For details see, V. Kataev et al., Phys. Rev. B 68, 140405(R) (2003). [2] A. Seidel et al., Phys. Rev. B 67, 020405(R) (2003). supported by DFG through SFB 608 TT 3.12 Mo 12:15 H18 Thermodynamic Properties of Layered Ruthenates — •J. Baier 1 , T. Zabel 1 , M. Kriener 1 , M. Reuther 1 , T. Lorenz 1 , A. Freimuth 1 , P. Steffens 1 , O. Friedt 1 , M. Braden 1 , A. Revcolevschi 2 , S. Nakatsuji 3 , and Y. Maeno 3 — 1 II. Physikalisches Institut, Universität zu Köln, Germany — 2 Laboratoire de Physico-Chimie de l‘Etat Solide, Universite Paris-Sud, Orsay, France — 3 Department of Physics, Kyoto University, Japan The phase diagram of Ca2−xSrxRuO4 presents a rich spectrum of distinct structural distortions, which are accompanied by drastic changes of the magnetic and electronic properties [1]. Ca-Doping drives the system from the spin-triplet superconductor Sr2RuO4 to the antiferromagnetic Mott-insulator Ca2RuO4. At x = 0.5, the low-temperature magnetic susceptibility is considerably increased and an unusually large Cp/T-value due to the evolution of a nearly ferromagnetic heavy-mass Fermi liquid is observed [2]. We find an anomalous, anisotropic thermal expansion for this compound. In a magnetic field, the anomalous thermal expansion and the large Cp/T-value are suppressed with an anisotropic field dependence. For lower x, an additional tilting of the RuO6 octahedra sets in and at x = 0.2 the susceptibility is again strongly reduced [2]. In high magnetic fields this compound is driven through a metamagnetic transition and the large susceptibility recovers. We observe a large magnetostriction during this metamagnetic transition. [1] O. Friedt et al., Phys. Rev. B 63 (2001) [2] S. Nakatsuji et al., Phys. Rev. Lett. 90 (2003) Supported by the DFG through SFB 608 TT 3.13 Mo 12:30 H18 Heat Transport in Low Dimensional Spin Systems — •C. Hess 1 , H. ElHaes 2 , P. Ribeiro 3 , B. Büchner 3 , F. Heidrich-Meisner 4 , W. Brenig 4 , M. Hücker 5 , U. Ammerahl 5 , and A. Revcolevschi 5 — 1 Department of Condensed Matter Physics, University of Geneva, Switzerland — 2 II. Physikalisches Institut, RWTH Aachen, Germany — 3 IFW Dresden, Germany — 4 Institut für Theoretische Physik, TU- Braunschweig, Germany — 5 Laboratoire de Physico-Chimie des Solides, Université Paris-Sud, France We present experimental results for the magnon thermal conductivity κmag of several low dimensional spin systems, like antiferromagnetic planes, ladders and chains. We focus on the quasi two dimensional antiferromagnet La2CuO4 and the spin ladder system (Sr, Ca, La)14Cu24O41, where scattering of the magnetic excitations on static defects, phonons, magnons and holes is analyzed on basis of a kinetic model. The analysis yields for example an intimate relation of magnetic and electronic transport channels in the spin ladders and in both systems a strict limitation of the magnon mean free path lmag by artificially induced non magnetic defects, i.e., lmag ≈ dZn−Zn at low temperatures, where dZn−Zn is the mean distance of doped Zn-ions in the low dimensional structures. The latter result is in stark contrast to recent model calculations for the heat transport in the spin ladders. TT 3.14 Mo 12:45 H18 Magnetic excitations in the low-dimensional quantum spin systems CaCu2O3 and Ba2Cu3O4Cl2 — •Eva Benckiser 1 , Markus Grüninger 1 , Tamara Nunner 2 , Thilo Kopp 2 , Chinnathambi Sekar 3 , and Gernot Krabbes 3 — 1 II. Physikalisches Institut, Universität zu Köln, Germany — 2 Experimentalphysik VI, Universität Augsburg, Germany — 3 IFW Dresden, Germany The magnetic excitations of CaCu2O3 and Ba2Cu3O4Cl2 are studied by means of phonon-assisted infrared absorption. CaCu2O3 has been discussed as a two-leg S=1/2 ladder with J⊥ ≪ J�. An analysis of the optical conductivity σleg(ω) for polarization parallel to the legs at 4K indeed yields J� ≈ 165 meV and a much smaller J⊥. However, comparison of σ(ω) for polarization parallel to the rungs and perpendicular to the ladders with the result of a DMRG calculation shows that the coupling perpendicular to the ladders is comparable to J⊥, i.e. that CaCu2O3 is not a ladder but rather a 3D system of weakly coupled chains. In the 2D cuprates, the large spectral weight in σ(ω) above the bimagnon-plus-phonon peak and the nature of the high-energy excitations are still under discussion. The 2D Cu3O4 layers in Ba2Cu3O4Cl2 contain the CuO2 square lattice plus a second Cu square lattice with a much weaker coupling constant J2. The spins of the two subsystems are decoupled from each other on the mean-field level. For ω ≫ J2 the compound represents a clean realization of an undoped CuO2 layer. We find that the high-energy spectral weight is larger than assumed previously. The temperature dependence of σ(ω) and a comparison with 1D systems strongly indicate a strong contribution from local, incoherent excitations. TT 4 Quantenflüssigkeiten, Bose-Einstein Kondensate, ultrakalte Atome, ... Zeit: Montag 10:00–12:15 Raum: H19 Hauptvortrag TT 4.1 Mo 10:00 H19 Kalte Atome in optischen Gittern — •Wilhelm Zwerger — Institut für Theoretische Physik, Universität Innsbruck, Technikerstr. 25, A-6020 Innsbruck, Kalte Atome in optischen Gittern stellen eine neue Klasse von Vielteilchensystemen dar, in denen die Stärke der Wechselwirkung durch Variation der Gittertiefe oder der Streulängen über einen weiten Bereich abstimmbar ist. Paradigmatische Modelle der Vielteilchenphysik, wie das Hubbard-Modell oder Luttinger-Flüssigkeiten sind daher experimentell realisierbar und geben Zugang zu komplexen Vielteilchenzuständen und den damit verbundenen Quantenphasenübergängen. Aufbauend auf dem Beispiel eines Mott-Hubbard Übergangs für Bosonen von Greiner et.al. wird ein Überblick über aktuelle Entwicklungen in diesem Gebiet ge- geben, insbesondere eindimensionale Systeme und die Perspektiven für Vielteilchenphysik mit Fermionischen kalten Atomen. TT 4.2 Mo 10:30 H19 Fluctuations and stability of superfluid turbulence in He-4 at mK temperatures — •Wilfried Schoepe — Fakultaet fuer Physik, Universitaet Regensburg Turbulent flow of superfluid helium-4 at mK temperatures around an oscillating microsphere is known to be unstable at low driving forces, switching intermittently between turbulent and laminar phases. The lifetimes of the turbulent phases are exponentially distributed and the mean lifetimes grow exponentially with the square of the driving force. These experimental results are attributed to statistical fluctuations of the vor-
Tiefe Temperaturen Montag ticity. As a model it is suggested that the turbulent state breaks down when a fluctuation crosses a threshold level. Applying Rice’s formula for the average level crossing per unit time of a stationary normal process gives information on the probability density function and the spectral bandwidth of the fluctuations. As a result a normal distribution is found and the standard deviation as well as the spectral bandwidth are determined quantitatively. In addition to superfluid turbulence this model may be applicable also to other instabilities which result from random fluctuations exceeding a certain threshold. TT 4.3 Mo 10:45 H19 Ground state properties and non-equilibrium dynamics of hard-core bosons confined on optical lattices — •Marcos Rigol Madrazo and Alejandro Muramatsu — Institut fuer Theoretische Physik III, Universitaet Stuttgart, Pfaffenwaldring 57, D-70550 Stuttgart, Germany We study by means of an exact numerical approach, a gas of hard core bosons (HCB) confined on optical lattices. The ground state properties of such systems are analyzed. Local incompressible phases appear in the system, like in the case of interacting soft-core bosons [1] and fermions [2,3]. The changes in momentum distribution function and in the natural orbitals (effective single particle states) introduced by the formation of such phases are analyzed. We also study non-equilibrium properties for those systems, which within our numerical approach can be obtained exactly for systems with ∼ 200 particles on lattices with ∼ 3000 sites. In particular we analyze the free expansion of the gas when it is released from the trap turning off the confining potential. We show that the expansion is non-trivial (as opposed to the fermionic case) and new features to be observed in the experiments are analyzed. [1] G. G. Batrouni, V. Rousseau, R. T. Scalettar, M. Rigol, A. Muramatsu,P. J. H. Denteneer, and M. Troyer, Phys. Rev. Lett. 89, 117203 (2002). [2] M. Rigol, A. Muramatsu, G. G. Batrouni, and R. T. Scalettar, Phys. Rev. Lett. 91, 130403 (2003). [3] M. Rigol and A. Muramatsu, cond-mat/0309670 (2003). TT 4.4 Mo 11:00 H19 Ultracold fermions and the SU(N) Hubbard model — •Carsten Honerkamp 1 and Walter Hofstetter 2 — 1 MPI Solid State Research, Stuttgart — 2 MIT, Cambridge, USA We investigate the fermionic SU(N) Hubbard model on the twodimensional square lattice for weak to moderate interaction strengths using one-loop renormalization group and mean-field methods. For the repulsive case U > 0 at half filling and small N the dominant tendency is towards breaking of the SU(N) symmetry. For N > 6 staggered flux order takes over as the dominant instability, in agreement with the large- N limit. Away from half filling for N = 3 the system rearranges the particle densities such that two flavors remain half filled by cannibalizing the third flavor. In the attractive case and odd N a full Fermi surface coexists with a superconductor in the ground state. These results may be relevant to future experiments with cold fermionic atoms in optical lattices. TT 4.5 Mo 11:15 H19 Self-energy and critical temperature of weakly interacting bosons — •Peter Kopietz, Sascha Ledowski, and Nils Hasselmann — Institut für Theoretische Physik, Universität Frankfurt, Robert-Mayer-Str. 8, 60054 Frankfurt/Main Using the exact renormalization group we calculate the momentumdependent self-energy Σ(k) at zero frequency of weakly interacting bosons at the critical temperature Tc of Bose-Einstein condensation in dimensions 3 ≤ D < 4. We obtain the complete crossover function interpolating between the critical regime k ≪ kc, where Σ(k) ∝ k 2−η , and the short-wavelength regime k ≫ kc, where Σ(k) ∝ k 2(D−3) in D > 3 and Σ(k) ∝ ln(k/kc) in D = 3. From our Σ(k) we find for the interaction- induced shift of Tc in three dimensions ∆Tc/Tc ≈ 1.23 an 1/3 , where a is the s-wave scattering length and n is the density [1]. [1] S. Ledowski, N. Hasselmann, and P. Kopietz, cond-mat/0311043. TT 4.6 Mo 11:30 H19 Reflectionless dynamics of 1D charge and spin modes in atomic traps — •Lars Kecke, Wolfgang Häusler, and Hermann Grabert — Physikalisches Institut, Albert- Ludwigs Univerität, Freiburg Gases of Fermionic atoms in cigar shaped, one-dimensional traps provide an ideal means to study the dynamics of correlated Fermi systems in the Tonks gas limit of repulsive contact interactions. The interaction strength can be tuned experimentally [1]. Based on the Tomonaga-Luttinger (TL) model we present calculations on the dynamics of charge and spin density waves. Particularly at the edge both modes show features that are strikingly different from the non-interacting case as well as from conventional TL dynamics. For example we find a suppression of reflections that should be experimentally observable. [1] T. Loftus et al PRL 88, 173201 (2002) TT 4.7 Mo 11:45 H19 Audio Demonstration of Quantum Oscillations: Phase Locking of Josephson Oscillations in superfluid 3He-B — •S.V. Pereverzev and G. Eska — Physikalisches Institut, Universität Bayreuth We report on a family of dynamic effects which were observed in superfluid 3He flow through a weak link (array of 65x65 holes of 150 nm dia. in a 50 nm SiN membrane). The flow was driven by a time dependent pressure difference (∆p(t)) to which an ac-modulation (paccos(ωt + θ)) was added. A self-trapping phase-locked state could be observed when the Josephson frequency (ωJ(t) = ∆p(t) ) and the ac-drive frequency ω merged ρκ0 (reverse AC-Josephson effect). This trapped state is a zero net current state with a nonzero pressure difference across the weak link. Close to this resonance the observed beat frequency ωJ − ω clearly indicates the presence of Josephson oscillations which can be heared. Low frequency oscillations around this quasi-equilibrium state were also observed, as well as Helmholtz oscillations around the zero pressure-difference equilibrium state. The frequencies of both of these oscillatory modes depended on amplitude and frequency of the ac-drive. For the pressure driven flow we measured unexpected high losses. The origin of these losses is unclear. TT 4.8 Mo 12:00 H19 Resonant Transport of Bose-Einstein Condensates — •Tobias Paul, Peter Schlagheck, and Klaus Richter — Institut für theoretische Physik, Universität Regensburg Due to the rapid progress of “atomic chip” technology [1], the implementation of experiments probing the propagation of Bose-Einstein condensates in mesoscopic waveguides becomes feasible. A particular interesting waveguide geometry is the double barrier structure created by a sequence of two constrictions, which can serve as a Fabry-Perot-like interferometer for the condensate [2]. In this context the question arises how the presence of repulsive interactions between the condensed atoms influences the transmission through this double barrier structure. Our numerical approach is based on the Gross–Pitaevskii equation and employs absorbing boundary conditions as well as an inhomogeneous source term in order to obtain a stationary flow of condensate through the guide. We show that the nonlinear interaction between the atoms leads to a significant modification of the positions and shapes of the resonance peaks as compared to the noninteracting case. [1] H. Ott et al., Phys. Rev. Lett. 87, 230401 (2001); J. Schmiedmayer et al., J. Mod. Optics 47, 2789 (2000); W. Hänsel et al., Nature 413, 498 (1999). [2] J. Fortagh and C. Zimmermann, Physik Journal, Juni 2003
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Symposium Organic and Hybrid System
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Symposium Physics of Foams Mittwoch
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Symposium Physics of Foams Mittwoch
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Symposium Quantum Shot Noise in Nan
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Symposium X-RAY Magneto-Optics Tage
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Symposium X-RAY Magneto-Optics Dien
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Lehrertage Regensburg Hauptvorträg
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A. D., Mirlin .................HL 1
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Breidenbach, Boris ........ AKB 50.
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Elli, Alexandra .............SYLS 3
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Greer, Lindsay ......... M 9.1, M 1
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Horn-von Hoegen, M. O 13.2, O 14.40
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Korn, Tobias ...............MA 13.6
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Martin, Tobias ............. MA 13.
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Partyka, Ewa ................ M 18.
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Rugeramigabo, Eddy Patrick O 14.38,
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Sihler, J. .................... DS
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Volz, K. .................... HL 44
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