Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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