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Tiefe Temperaturen Dienstag The preparation, manipulation and detection of single spin states are the essential prerequisites for spin based quantum computation. The coupling of a single C13 spin (I=1/2) to the ground state triplet spin (S=1) of a single nitrogen-vacancy defect center (NV-center)in diamond forms a single 2-qubit system. The joint approach of single molecule spectroscopy and optically detected magnetic resonance (ODMR) allows to detect optically individual NV-centers and to manipulate the spin subsystem of the defect. Coherent oscillations of the triplet spin in a single NV-Center have been detected. Further pulsed ODMR sequences, derived from optical detected electron nuclear double resonance experiments, allows the coherent control of the coupled spin states. As a first quantum computation operation the conditional rotation gate (CROT) has been implemented. The poster presents the measurements and discusses the limitations due to coherence decay. TT 17.27 Di 14:30 Poster A Towards an Autonomous Quantum Thermodyamic Machine — •Friedemann Tonner und Günter Mahler — Institut für Theoretische Physik 1, Universität Stuttgart, Pfaffenwaldring 57, D-70550 Stuttgart On a fundamental level thermodynamic machines necessarily consist of quantum mechanical parts. Here we address quantum mechanical analogs to each functional part of a thermodynamic machine. Thus we construct time-independent Hamiltonians for the gas system, the work variable and the control system responsible for driving the thermodynamic process, normally controlled from the outside. Baths are dealt with in Markov approximation. We are interested not in quantum mechanical modeling of existing (classical) machines, but rather in exploring the small system (quantum) limit: how small can a machine be made to still exhibit machine functions? TT 17.28 Di 14:30 Poster A Schrödinger-dynamics of a spin-chain in contact with a quantum environment — •Markus Henrich, Michael Hartmann, Mathias Michel, and Günter Mahler — Institut für Theoretische Physik 1, Universität Stuttgart, Pfaffenwaldring 57, D-70550 Stuttgart We study the exact Schrödinger-dynamics of a spin-chain with nearestneighbour interaction coupled to a finite quantum environment. The relaxation behavior of the spin-chain is analyzed for two coupling topologies; 1. all spins are directly coupled to the environment, 2. only one edge of the spin-chain is coupled to the environment. Various coupling strengths between the spins as well as various initial states are considered. We then analyze the conditions under which a thermodynamical description should become appropriate for the entire spin-system or even for the induvidual spins. TT 17.29 Di 14:30 Poster A Viscous Transport in Dirty Fermi Superfluids — •Dietrich Einzel 1 and Jeevak M. Parpia 2 — 1 Walther-Meissner-Institut, Bayerische Akademie der Wissenschaften, 85748 Garching — 2 Dept. of Physics, Cornell University, Ithaca, NY 14853, USA The transport theory of clean Fermi superfluids like 3 He–A,B is generalized to include strong elastic scattering from impurities represented by a system of low density silica arogel strands. The dynamics of the aerogel system is taken into account within a collision–drag model. In particular, we calculate for the first time the viscosity of superfluid 3 He–B in the presence of impurity scattering both in the Born and the unitary limit. The shear viscosity dominates the attenuation of transverse sound, the general dispersion relation of which is also provided by our theory. The observability of the shear viscosity is discussed in context with recent torsional oscillator experiments. TT 17.30 Di 14:30 Poster A Pressure Driven 3 He Flow Through Submicron Sized Apertures — •S.V. Pereverzev and G. Eska — Physikalisches Institut, Universität Bayreuth The flow of liquid 3 He through two different weak link structures was investigated at temperatures of T< 1 mK to 1 K by measuring the characteristic time τ which was needed for pressure equilibration between two volumes connected by the weak links. For the flow through a regular structure of 65x65 holes of 150 nm dia. in a 50 nm thick SiN membrane we observed the expected T-dependence and the transition from Knudsen to viscous flow behavior. To the contrary, no T-dependence was found for normal fluid 3 He-flow through 10 5 holes of 15 nm diameter, statistically distributed over a 14 nm thick nitrocellulose film. Below the superfluid transition the relaxation rate (1/τ ∼flow-channel conductance) increased by orders of magnitude for both types of weak links. Our data are in qualitative agreement with experiments by other groups. We present a model which describes our normal flow results quantitatively for the 150 nm aperture, but which does not explain the flow through the 15 nm holes. TT 17.31 Di 14:30 Poster A Light propagation and random lasing — •Andreas Lubatsch and Hans Kroha — Physikalisches Institut, Universitaet Bonn We present caculations and numerical results for light propagation in disordered media. We consider vector waves passing through a system of randomly distributed Mie - scatterers. The scaterers themselves can consist of optical active media. We present as well results for such systems, which are known as random lasers. In order to find the results, we calculated the necessary transport properties including e.g. the exact Ward Identity and the diffusion constant. TT 17.32 Di 14:30 Poster A Channel analysis of electrical conductance through a Zn single-atom contact — •Michael Häfner, Jan Heurich, Juan-Carlos Cuevas und Gerd Schön — Institut für Theoretische Festkörperphysik, Universität Karlsruhe, 76128 Karlsruhe Today it is possible to manipulate atomic-sized structures in a controlled way. Special attention is payed to the electronic transport properties of single-atom contacts. For noble and s-p like metals the conduction is carried by the s-band (one channel) and the s- and p-bands (up to four channels) respectively. Scheer et al. have recently measured the conductance of Zn single-atom contacts. As Zn is intermediate between noble and s-p like metals it constitutes an excellent testbed for the detailed study of the interplay between electronic configuration and conduction properties in this regime. In this work we present a theoretical analysis of the experiment using tight binding transport calculations. This approach allows us to show how the conduction channels arise from the atomic orbitals and elucidate which specific properties of the individual orbitals determine their contribution to the current. For the case of Zn single-atom contacts we find a typical total transmission of ∼ 0.6 in good agreement with the experiment. In contrast to the noble or s-p like metals, the current is predominantly carried by two channels which can be related to a combination of the s and p valence bands of Zn. TT 18 Supraleitung: Tunneln, Josephson-Kontakte, SQUIDs Zeit: Mittwoch 14:30–16:30 Raum: H20 TT 18.1 Mi 14:30 H20 Electron tunneling into superconducting MgB2 — •J. Geerk, R. Schneider, A. Zaitsev, R. Heid, and G. Linker — Forschungszentrum Karlsruhe, Institut für Festkörperphysik We have prepared tunnel junctions of the sandwich-type on superconducting thin films of MgB2. The films were prepared by physical vapor deposition from an evaporation source for magnesium and a sputtering source for boron with Tc values near 33 K. The tunnel junctions showed an energy gap between 2.5 and 3.0 meV and phonon structures in the reduced density of states with a strength of about 0.8%. The inversion of the tunnel data using standard single-band Eliashberg equations revealed an Eliashberg function with 3 distinct peaks at 40, 60 and 90 meV. It can be deduced that the boron-like phonons (60 and 90 meV) couple about 3 times stronger than the magnesium like phonons (40 meV). The strong peak due to the E2g-mode near 70 meV which is predicted by several theoretical calculations could not be detected in the tunnel data.
Tiefe Temperaturen Mittwoch TT 18.2 Mi 14:45 H20 Experimental Realization of all High-Tc dc π/2-SQUIDs — •Christof Schneider, German Hammerl, Rainer Held, Klaus Wiedenmann, and Jochen Mannhart — Experimentalphysik VI, Universität Augsburg In the presentation, we will report on the realization of all high-Tc π/2-SQUIDs. The characteristics of the π/2-SQUIDs, which were fabricated using YBa2Cu3O7−δ thin films grown on tetracrystalline substrates will be presented and compared with the properties of standard high-Tc SQUIDs. TT 18.3 Mi 15:00 H20 Imaging of Josephson Current Distribution in YBa2Cu3O7-Nb Zigzag Junctions — •D. Dönitz 1 , E. Goldobin 1 , R. Straub 1 , R. Kleiner 1 , D. Koelle 1 , H.J.H. Smilde 2 , Ariando 2 , H. Hilgenkamp 2 , and H. Rogalla 2 — 1 Universität Tübingen, Physikalisches Institut – Experimentalphysik II, Auf der Morgenstelle 14, D-72076 Tübingen, Germany — 2 Low Temperature Division, Faculty of Science and Technolgoy and MESA+ Research Institute, University of Twente, P.O. Box 217, 7500 AE Enschede, The Netherlands We used low temperature scanning electron microscopy (LTSEM) to image the supercurrent distribution in zigzag YBa2Cu3O7 (YBCO)–Nb ramp edge Josephson junctions. These junctions consist of several artificial facets of length a ≤ λJ and alternating orientation along the in-plane crystallographic axes of the YBCO film. At zero applied magnetic field we clearly observed the reversal of the direction of the Josephson current flowing through neighboring facets. This is a direct visualization of the opposite sign of the critical current in neighboring facets, i.e. they can be considered as 0 and π junctions. This constitutes direct imaging of the sign change in the phase of the d x 2 −y 2 order parameter symmetry in YBCO. We performed numerical simulations of the sine–Gordon model which showed that for our particular geometry the phase profile along the zigzag junctions corresponds to a compressed chain of antiferromagnetically ordered semifluxons. At the matching field, for which the critical current is maximum, the simulations predict a supercurrent distribution which has the same sign and an arc–like profile in all facets. This prediction is directly confirmed by LTSEM. TT 18.4 Mi 15:15 H20 Doping dependence of pseudogap and superconductivity in electron doped high-temperature-superconductors: results from tunneling spectroscopy — •B. Welter 1 , L. Alff 1 , Y. Krockenberger 1 , M. Naito 2 , and R. Gross 1 — 1 Walther-Meissner-Institut, Bayerische Akademie der Wissenschaften, Walther-Meissner-Str. 8, 85748 Garching, Germany — 2 NTT Basic Research Laboratories, Atsugi, Japan Studying the influence of doping on the characteristics of oxide superconductors is essential to both the understanding of the underlying physics and the development of new applications. Here, we report on tunneling spectroscopy measurements on grain boundary junctions of electron doped high-temperature superconductors La2−xCexCuO4, Pr2−xCexCuO4 and Nd2−xCexCuO4 with different Ce concentrations around optimal doping. We focus on the pronounced depletion in the density of states near EF observed in the normal state above Bc2 and its evolution with temperature, magnetic field and doping [1]. Considerations concerning the conservation of states rule even indicate a coexistence of this pseudogap regime and the superconducting state.[2] [1] L. Alff, Y. Krockenberger, B. Welter, M. Schonecke, R. Gross, D. Manske and M. Naito, Nature 422, 698 (2003) [2] B. Welter, Y. Krockenberger, L. Alff, M. Naito und R. Gross, to appear in Physica C TT 18.5 Mi 15:30 H20 STM structure analysis of bismuth high-TC crystals depending on the bias voltage — •Hendrik Glowatzki, Torsten Stemmler, Johannes Zeggel, Alicia Krapf, Christoph Janowitz, and Recardo Manzke — Institut f. Physik, Humboldt-Universität zu Berlin, Newtonstr. 15, 12489 Berlin A detailed structural analysis of single and double layered bismuth single crystals (BSCCO) has been performed by Scanning Tunneling Microscopy (STM). Because of the special layered configuration of these superconductors, containing semiconducting, insulating and the superconducting metallic layers, we obtain different atomic images depending on the applied tunneling voltage. In particular, semiconducting layers will be invisible for bias voltages below its gap energy /1/. So it has become possible to observe not only the surface layer but also deeper CuO2-layers which cause high-TC superconductivity. The results can be understood from the particular crystal structure of BSCCO. [1] Oda, M. et al. Phys. Rev. B 53, 2253 (1995) TT 18.6 Mi 15:45 H20 Cavity resonances in Bi2Sr2CaCu2O8 intrinsic Josephson junction stacks under low frequency microwave irradiation — •Tobias Clauss, Takashi Uchida, Michael Mößle, Dieter Koelle, and Reinhold Kleiner — Universität Tübingen, Physikalisches Institut - Experimentalphysik II, Auf der Morgenstelle 14, 72076 Tübingen One important problem towards the realization of THz oscillators from intrinsic Josephson junction stacks is to make the junctions in the stack to oscillate in-phase. One possibility to generate such oscillations is to excite cavity resonances by collective motion of Josephson fluxons in the stack. So far, cavity resonances have only been observed for Bi2Sr2CaCu2O8 stacks at high external magnetic fields. We have investigated single crystal Bi2Sr2CaCu2O8 stacks at zero magnetic field under microwave irradiation with frequencies between 2 and 25 GHz. Measured current voltage characteristics show structures which can be attributed to cavity resonances. Using low temperature scanning electron microscopy to image the current distribution in the stack we find clear cavity resonances with wavelengths of some µm. We believe that the resonances are excited by the collective motion of vortex-antivortex pairs generated by the external microwave field. TT 18.7 Mi 16:00 H20 Intrinsic Josephson Effects in RuSr2GdCu2O8 — •Timo Nachtrab 1 , D. Koelle 1 , R. Kleiner 1 , C. T. Lin 2 , and C. Bernhard 2 — 1 Universität Tübingen, Physikalisches Institut -Experimentalphysik II, Auf der Morgenstelle 14, 72076 Tübingen, Germany — 2 Max-Planck- Institut für Festkörperforschung, Heisenbergstrasse 1, 70569 Stuttgart, Germany We report on electrical transport measurements on single crystals of RuSr2GdCu2O8(Ru1212). The material shows coexistence of magnetic ordering (Tm ≈ 130 K) and superconductivity (Tc ≈ 55 K) at low temperatures. The crystal structure consists of alternating RuO2 layers (with a weak ferromagnetic (F) component in-plane) and superconducting (S) CuO2 layers, separated by insulating (I) layers of SrO. Ru1212 thus forms an intrinsic SIFIS multilayer structure. For transport perpendicular to the planes an intrinsic Josephson effect as, e.g., in Bi2Sr2CaCu2O8+δ (Bi2212) has been predicted. In addition, the magnetic component inside the barrier might provoke interesting phenomena like π-phases in the superconducting order parameter. We measured the interlayer current transport in micron-sized Ru1212 single crystals in magnetic fields up to 7T and temperatures between 4.2K and 300K. The system shows a clear intrinsic Josephson effect, e.g. the typical multi-branched current-voltage characteristics known from high-Tc cuprates. Our magnetic field measurements reveal that fluxon motion takes place in a very similar fashion as in Bi2212. So far, however, we did not observe any unconventional behavior due to the magnetism of the RuO2 layers. TT 18.8 Mi 16:15 H20 Charge-imbalance relaxation rate in layered d-wave superconductors — •Joachim Keller and Dmitri Ryndyk — Institut für Theoretische Physik, Universität Regensburg, 93040 Regensburg Intrinsic (inter-layer) Josephson effect in layered d-wave superconductors is accompanied by static and oscillating charge fluctuations on the layers. In a system of weakly coupled very thin atomic layers, such charge fluctuations may lead to non-equilibrium effects described by a shift of the chemical potential of the condensate and a charge imbalance between electron- and hole-like quasiparticles. We have developed the microscopic theory based on the nonequilibrium Green function method and calculated static and high-frequency charge imbalance relaxation rates in dwave superconductors (which are determined at low temperatures by elastic scattering). 16:30 Pause
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Lehrertage Regensburg Hauptvorträg
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A. D., Mirlin .................HL 1
Page 521 and 522:
Breidenbach, Boris ........ AKB 50.
Page 523 and 524:
Elli, Alexandra .............SYLS 3
Page 525 and 526:
Greer, Lindsay ......... M 9.1, M 1
Page 527 and 528:
Horn-von Hoegen, M. O 13.2, O 14.40
Page 529 and 530:
Korn, Tobias ...............MA 13.6
Page 531 and 532:
Martin, Tobias ............. MA 13.
Page 533 and 534:
Partyka, Ewa ................ M 18.
Page 535 and 536:
Rugeramigabo, Eddy Patrick O 14.38,
Page 537 and 538:
Sihler, J. .................... DS
Page 539 and 540:
Volz, K. .................... HL 44
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