Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Tiefe Temperaturen Freitag<br />
beobachtet, bei der Spannungssprünge in den I-U-Kennlinien aufgrund<br />
von Larkin-Ovchinikov-Vortex Instabilitäten auftreten. Die experimentell<br />
bestimmten Matching-Felder werden im Zusammenhang mit bestehenden<br />
Theorien für dünne Schichten diskutiert.<br />
TT 31.8 Fr 12:00 H20<br />
Advanced manipulation of substrates for growth induced pinning<br />
in YBCO thin films — •S. Brück 1 , J. Albrecht 1,2 , S. Leonhardt<br />
2 , R. Spolenak 1 , G. Cristiani 2 , H.–U. Habermeier 2 , and G.<br />
Schütz 1 — 1 Max-Planck-Institut für Metallforschung, Heisenbergstr.<br />
3, D-70569 Stuttgart — 2 Max-Planck-Institut für Festkörperforschung,<br />
Heisenbergstr. 1, D-70569 Stuttgart<br />
One way to enhance flux pinning and thus the critical current density<br />
in YBCO thin films is by modifying the substrates’ surface topography<br />
[1,2]. Irradiation with a focused beam of gallium ions (FIB) creates dotlike<br />
structures which induce pinning sites in the superconductor during<br />
film growth. To enhance the density of these structures it is necessary to<br />
prevent surface charging, which can be achieved by using substrates with<br />
a higher conductivity. We show AFM images of the microstructures and<br />
quantitative magnetooptical measurements of YBCO thin films grown on<br />
such sophisticated substrates. It is found, that the critical current density<br />
can be enhanced substantially by lateral size reduction of the created<br />
structures.<br />
[1] S. Leonhardt, J. Albrecht, R. Warthmann, H.-U. Habermeier and<br />
H. Kronmüller, Physica C 341-348, 1979-1980 (2000)<br />
[2] J. Albrecht, S. Leonhardt, H.-U. Habermeier, S. Brück, R. Spolenak<br />
and H. Kronmüller, Physica C, in Press<br />
TT 31.9 Fr 12:15 H20<br />
Competitive localization of vortex lines or interacting bosons<br />
by a defect — •Jan Kierfeld 1 and Valerii Vinokur 2 — 1 MPI<br />
für Kolloid- und Grenzflächenforschung, 14424 Potsdam — 2 Materials<br />
Science Division, Argonne National Laboratory<br />
We present a theory describing the localization of N three-dimensional<br />
vortex lines or two-dimensional bosons with short-ranged repulsive interaction<br />
which are competing for a single columnar defect or potential<br />
well. For N=2 we use a necklace model formulation to find a delocalization<br />
transition between two different states with a single bound particle.<br />
The transition is characterized by the onset of particle exchange on the<br />
defect. For strong repulsive interaction between vortex lines a permutation<br />
symmetry is broken and the potential well is occupied by the same<br />
particle at all times. For decreasing repulsion or increasing temperature<br />
a transition into a different bound state takes place in which the particles<br />
occupy the potential well alternately. A generalization of this transition<br />
to arbitrary vortex number N is proposed.<br />
TT 31.10 Fr 12:30 H20<br />
Enhanced Magnetic Flux Pinning of Nanocrystalline Mechanically<br />
Alloyed Bulk MgB2 by Stoichiometry Variation and Doping<br />
— •Olaf Perner 1 , Jürgen Eckert 2 , Günter Fuchs 1 , Konstantin<br />
Nenkov 1 , Bernhard Holzapfel 1 , and Ludwig Schultz 1<br />
— 1 Leibniz-Institut für Festkörper- und Werkstoffforschung Dresden, PF<br />
270116, D-01171 Dresden — 2 TU Darmstadt, Petersenstr. 23, D-64287<br />
Darmstadt<br />
In order to overcome the poor intrinsic properties of MgB2 concerning<br />
the low upper critical field and to obtain an enhancement of the magnetic<br />
flux pinning a combination of microstructure optimization as well<br />
as chemical variation of the pure MgB2 compound were chosen.<br />
Starting from the elements Mg and B, the phase formation was realized<br />
by the mechanical alloying technique receiving a partially reacted<br />
MgB2 powder with grain sizes of about 10 nm. Short uniaxial hot pressing<br />
under vacuum led to phase pure highly densified nanocrystalline bulk<br />
samples with low impurity content. The variation of the stoichiometry by<br />
increasing and reducing the Mg content by up to 10 wt.% as well as the<br />
doping with various concentrations of SiO2 and MgO leads to increased<br />
pinning forces Fp compared to the stoichiometric composition.<br />
The MgB2 bulk sample with a Mg excess of 10 wt.% shows an improved<br />
critical temperature Tc of 36.0 K and a critical current density jc<br />
of about 10 6 A/cm 2 at 7.5 K in self field whereas Mg deficit of 10 wt.%<br />
enhances the upper critical field Hc2 (9 T at 20 K). Doping with SiO2<br />
which improves significantly Hc2 and jc reveals more effective than with<br />
MgO. Microstructure investigations will be presented.<br />
TT 32 Theoretische Modelierung von Materialien mit korrelierten Elektronen<br />
Zeit: Freitag 10:15–13:00 Raum: H18<br />
TT 32.1 Fr 10:15 H18<br />
Quasiparticles from quantum Monte Carlo: Effective mass and<br />
Wilson ratio for K3C60 — •Erik Koch and Olle Gunnarsson —<br />
Max-Planck-Institut für Festkörperforschung, Stuttgart<br />
Taking advantage of the fixed-node approximation to stabilize excited<br />
states, we calculate quasiparticle energies by quantum Monte Carlo. We<br />
apply this approach to a model describing K3C60 and show that it works<br />
surprisingly well. We determine how the quasiparticle dispersion changes<br />
with increasing correlation and compare to the many-body enhancement<br />
of the Pauli susceptibility. While the self-energies for our model seem<br />
to depend only weakly on the momentum (and band-index), we find a<br />
Wilson ration that appears to behave qualitatively different from what<br />
is expected from dynamical mean-field theory.<br />
TT 32.2 Fr 10:30 H18<br />
A wavefunction-based quantum chemical method for infinite<br />
systems — •Beate Paulus — Max-Planck-Institut für Physik komplexer<br />
Systeme, Nöthnitzer Straße 38, D-01187 Dresden<br />
Wave-function based quantum chemical methods are applied to the<br />
infinite system using an incremental scheme to partitioning the correlation<br />
energy. After the success for a wide range of semiconductors [1] and<br />
insulators even such weakly bound as rare gas crystals [2], the method<br />
is extended to strongly correlated metallic systems [3]. As example we<br />
present the cohesive energy of mercury, where the binding is entirely due<br />
to correlations. [1] B. Paulus, P. Fulde and H. Stoll,Phys. Rev. B 54<br />
(1996) 2556 [2] K. Rosciszewski, B. Paulus, P. Fulde, and H. Stoll,Phys.<br />
Rev. B 60 (1999) 7905 [3] B. Paulus, Chem. Phys. Lett. 371 (2003) 7<br />
TT 32.3 Fr 10:45 H18<br />
TiOCl, an orbital-ordered system? — •Roser Valenti 1 , T. Saha-<br />
Dasgupta 2 , Helge Rosner 3 , and Claudius Gros 4 — 1 Institut für<br />
Theoretische Physik, Universität Frankfurt, D-60054 Frankfurt — 2 S.N.<br />
Bose National Centre for Basic Sciences, Kolkata 700098, India — 3 Max-<br />
Planck Institute for Chemical Physics of Solids, D-01187 Dresden —<br />
4 Theoretische Physik, Universität des Saarlandes, D-66041 Saarbrücken<br />
We present first principles density functional calculations and downfolding<br />
studies of the electronic and magnetic properties of the layered<br />
quantum spin system TiOCl. We attempt to clarify the concept of orbital<br />
ordering in this material and discuss existing studies. An analysis<br />
of the electronic structure of slightly distorted structures according to<br />
the phononic modes allowed in this material suggests that this system is<br />
subject to large orbital fluctuations driven by the electron-phonon coupling.<br />
Based on these results, we propose a microscopic explanation of<br />
the behavior of TiOCl at lower temperatures.<br />
TT 32.4 Fr 11:00 H18<br />
Hartree-Fock-Approximation und Berücksichtigung von<br />
Abschirm-Effekten in Ab-Initio-Bandstruktur-Berechnungen<br />
— •Olaf Peschel 1 , Ilan Schnell 2 und Gerd Czycholl 1 —<br />
1 Universität Bremen, Institut für Theoretische Physik — 2 Los Alamos<br />
National Laboratory, Theoretical Division<br />
Wir gehen von den Bloch-Wellenfunktionen einer DFT-Hartree-<br />
Rechnung (ohne Austausch-Korrelationspotential) aus, die wir zu<br />
maximal lokalisierten Wannier-Funktionen Transformieren. Bezüglich<br />
dieser Basis berechnen wir die Hopping- und Coulomb-Matrixelemente<br />
des Hamilton-Operators in Zweiter Quantisierung und führen eine<br />
selbstkonsistente Hartree-Fock-Rechnung durch. Alternativ können<br />
wir eine Hartree-Fock-(HFA)-Rechnung mit bezüglich der Bloch-Basis<br />
berechneten Matrixelementen durchführen.<br />
Um über die HFA hinauszugehen und Abschirmeffekte zu berücksichtigen,<br />
berechnen wir die Suszeptibilität in verallgemeinerter Lindhard-