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Plenarvorträge - DPG-Tagungen

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Tiefe Temperaturen Montag<br />

YBCO-Filme der Dimension 10mm x 42mm x 300nm. Unterhalb des<br />

Films befand sich eine supraleitende Pfannkuchenspule an welche RF-<br />

Pulse angelegt wurden. War der an der Probe angelegte Bias-Strom ausreichend<br />

hoch, konnte damit der Übergang in die Normalleitung ausgelöst<br />

werden. Mittels des magnetooptischen Verfahrens war es möglich<br />

die Flussdichteverteilung in dem YBCO-Streifen vor, während und nach<br />

dem Schaltvorgang zu beobachten und somit Rückschlüsse auf die jeweiligen<br />

Stromverteilungen zu ziehen. Als Ergebnis werden magnetooptische<br />

Aufnahmen und ein theoretisches Modell des RF-induzierten Schaltvorgangs<br />

vorgestellt.<br />

TT 8.32 Mo 14:30 Poster A<br />

Magnetic Properties of YBa2Cu3O7 Ring Structures —<br />

•K. Schindler 1 , M. Ziese 1 , P. Esquinazi 1 , H. Hochmuth 2 ,<br />

M. Lorenz 2 , E. Salamatin 3 , and K. Zimmer 3 — 1 Division of<br />

Superconductivity and Magnetism, University of Leipzig, 04103 Leipzig.<br />

— 2 Semiconductor Physics Group, University of Leipzig, 04103 Leipzig.<br />

— 3 IOM, Institute for Surface Modification, 04318 Leipzig.<br />

YBa2Cu3O7 (YBCO) films were grown by pulsed laser deposition on<br />

CeO2-buffered r-plane sapphire substrates. Film thickness was 260 nm;<br />

the films were covered with a gold layer of 220 nm. From a single 3 inch<br />

wafer various ring structures were fabricated using photolithographical<br />

techniques and subsequent etching with either an Excimer laser or an<br />

ultrafast Ti:sapphire laser, respectively. The magnetic properties of the<br />

YBCO ring structures were investigated by ac-susceptibility and SQUID<br />

magnetometry. In order to quantify and assess the material damage introduced<br />

by the different etching techniques, the critical current density<br />

of 12 single rings with 2 mm outer diameter and ring widths between 15<br />

and 110 µm was determined by magnetic field dependent ac-susceptibility<br />

measurements. The complex susceptibility of the rings at least up to the<br />

13th harmonic could be accurately modelled within a critical state model.<br />

The values of the critical current density extracted did not show a systematic<br />

dependence on the patterning technique. Furthermore, structures<br />

with 1024 rings of outer diameter 20 µm and ring width 1 and 2 µm were<br />

investigated. FC-, ZFC- and remanent magnetization measurements were<br />

used to determine the volume of shielded material. The data will be further<br />

discussed within a critical state model.<br />

TT 8.33 Mo 14:30 Poster A<br />

Frequency dependence up to microwave frequencies of the abplane<br />

conductivity peak near Tc of YBa2Cu2O7−δ — •D. Görlitz<br />

and J. Kötzler — Institut f. Angewandte Physik, Univ. Hamburg, D-<br />

20355 Hamburg<br />

The linear suceptibility χ ′ − iχ ′′ of d=50-600 nm thin films has been<br />

measured between 30mHz and 22GHz in ac-fields perpendicular to the<br />

CuO2-planes. For frequencies up to 800 kHz mutual induction techniques<br />

were employed, while between 0.45 and 22 GHz the complex resonance<br />

frequency, ˜ fr = fr + i∆f, of helical resonators and of cylindrical cavities<br />

was determined. The complex shifts δ ˜ fr = ˜ fr(T) − ˜ fr(0) are proportional<br />

to the dynamic susceptibility χ(ω), and DC-susceptibilities were<br />

employed to calibrate δfr. The ab-plane conductivity σ(ω) = σ ′ − iσ ′′<br />

is determined from χ(ω) by means of an exact inversion routine [1].<br />

The loss component σ ′ shows a peak at a temperature Tω near Tc, and<br />

the peak temperatures Tω exhibit an Arrhenius behaviour. Using the inverse<br />

kinetic inductivity determined from σ ′′ ,(µ0Lk(T)) −1 = ωσ ′′ (T, ω),<br />

the Arrhenius barriers are related to the nucleation energy of vortex<br />

cores threading the film. These barriers are found to disappear at T0,<br />

which is distinctly above the true critical temperature Tc, also extracted<br />

from L −1<br />

k (T)[2]. At the largest frequency, 21.3 GHz, the σ ′ -peak becomes<br />

strongly suppressed since Tω approaches T0.<br />

[1] J. Kötzler et al., Phys.Rev. B 50, 3384 (1994)<br />

[2] J. Kötzler et al., Phys.Rev.Lett. 87, 127005 (2001) and 89,149704<br />

(2002)<br />

TT 8.34 Mo 14:30 Poster A<br />

Evidence for a percolation-driven transition to coherent surface<br />

superconductivity — •Lars von Sawilski, Sara Casalbuoni, and<br />

Jürgen Kötzler — Institut für Angewandte Physik und Zentrum<br />

für Mikrostrukturforschung, Universität Hamburg, Jungiusstrasse 11, D-<br />

20355 Hamburg, Germany<br />

Above the upper critical field Hc2 we have investigated the field dependences<br />

of the surface conductance, G ′ − iG ′′ , and the critical current<br />

Jc of different treated Niobium cylinders: as grown, chemically and electrolytically<br />

polished. The low frequency limits of G ′ (H) and G ′′ (H) and<br />

of Jc(H) display power-law singularities, defining a transition to coherent<br />

surface superconductivity at H c c3 > Hc2. The critical exponents as well as<br />

the dynamical scaling of G ′ − iG ′′ studied between 0.1 Hz and 1 MHz are<br />

consistent with predictions for a two-dimensional percolation transition.<br />

Relating H c c3 to the conventional onset field for surface superconductivity<br />

Hc3, we find H c c3 /Hc3 = 0.81. Surprisingly, this ratio turns out to<br />

be independent of significant variations of Hc3 due to differently treated<br />

surfaces. This points to a new universal relation between the nucleation<br />

and the onset of long-range coherent surface superconductivity.<br />

TT 8.35 Mo 14:30 Poster A<br />

Influence of Fermi surface topology on the quasiparticle spectrum<br />

in the vortex state — •Siegfried Graser, Thomas Dahm,<br />

and Nils Schopohl — Institut für Theoretische Physik, Universität<br />

Tübingen, Auf der Morgenstelle 14, D-72076 Tübingen<br />

We study the influence of Fermi surface topology on the quasiparticle<br />

density of states in the vortex state of type II superconductors. We<br />

observe that the field dependence and the shape of the momentum and<br />

spatially averaged density of states is affected significantly by the topology<br />

of the Fermi surface. We show that this behavior can be understood<br />

in terms of characteristic Fermi surface functions and that an important<br />

role is played by the number of points on the Fermi surface at which the<br />

Fermi velocity is directed parallel to the magnetic field. A critical comparison<br />

is made with a broadened BCS type density of states, that has been<br />

used frequently in analysis of tunneling data. We suggest a new formula<br />

as a replacement for the broadened BCS model for the special case of a<br />

cylindrical Fermi surface. We apply our results to the two gap superconductor<br />

MgB2 and show that in this particular case the field dependence<br />

of the partial densities of states of the two gaps behaves very differently<br />

due to the different topologies of the corresponding Fermi surfaces, in<br />

qualitative agreement with recent tunneling experiments.<br />

TT 8.36 Mo 14:30 Poster A<br />

Local Quasiparticle Density of States in unconventional Type-<br />

II Superconductors — •Christian Iniotakis and Nils Schopohl<br />

— Institut für Theoretische Physik, Universität Tübingen, Auf der Morgenstelle<br />

14, D-72076 Tübingen<br />

Our aim is to calculate the quasiclassical propagator in unconventional<br />

(d-wave) superconductors in the vortex state. We assume a clean and<br />

homogeneous superconductor. Near the phase transition at Hc2 the spacial<br />

variation of the gap function is given by the well-known Abrikosov<br />

solution. Concentrating on the quadratic and hexagonal vortex lattice<br />

we present calculations of the local quasiparticle density of states. Our<br />

results have been achieved by using the Riccati-parametrization of the<br />

quasiclassical Eilenberger theory. Additionally, basic symmetry relations<br />

of the vortex lattice have been taken into account.<br />

TT 8.37 Mo 14:30 Poster A<br />

Mirage phenomena in quantum corrals of s-wave superconductors<br />

— •Markus Schmid and Arno P. Kampf — Theortical<br />

Physics III, Center for Electronic Correlations and Magnetism, Institute<br />

of Physics, University of Augsburg, 86135 Augsburg<br />

We investigate the local pairing amplitude and the local density of<br />

states (LDOS) for an s-wave superconductor in an elliptic quantum corral.<br />

Using a T-matrix analysis we explore the spatial structure of the<br />

LDOS in the presence of a single non-magnetic impurity and observe a<br />

variety of quantum mirage phenomena. In particular, we discuss mirage<br />

effects for localized impurity bound states and analyze the interference<br />

patterns for the scattering processes from two impurities in the quantum<br />

corral.<br />

TT 8.38 Mo 14:30 Poster A<br />

Extraction of the nonlinear response function from intermodulation<br />

distortion experiments and application to<br />

high-temperature superconductor resonators — •Roland<br />

Hott, Alexander Zaitsev, and Rudolf Schneider —<br />

Forschungszentrum Karlsruhe, Institut für Festkörperphysik, P.O.B.<br />

3640, D-76021 Karlsruhe, Germany<br />

We present a general scheme how to extract the response function<br />

Z(H) = �<br />

m ZmHm for a nonlinear reaction of a quantity<br />

E(H) = Z(H)H on an input H from two-tone intermodulation distortion<br />

(IMD) experiments using a time-dependent excitation H(t) =<br />

h cos(ω0t) cos(δ0t). We applied this method with success to hightemperature<br />

superconductor (HTS) rf resonators to identify here the<br />

mechanism of nonlinear signal distortions. Comparison of the experimental<br />

3rd-order IMD I3(pcirc) measured as function of rf power pcirc

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