Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
Tiefe Temperaturen Mittwoch<br />
is a consequence of the Lang-Firsov transformation, the combination of<br />
these elements enables us to perform efficient simulations for a wide range<br />
of temperature, phonon frequency and electron-phonon coupling in one<br />
to three dimensions, and on clusters large enough to avoid significant<br />
finite-size effects. The algorithm is employed to investigate the problem<br />
of small polaron formation in the Holstein model, and comparison with<br />
exact results and with existing work is made. Moreover, the new ideas<br />
presented here can also be applied to the many-electron case.<br />
TT 24.5 Mi 14:30 Poster A<br />
Variational cluster approach to extended Hubbard models at<br />
half filling — •Markus Aichhorn 1 , Hans Gerd Evertz 1 , Wolfgang<br />
von der Linden 1 , and Michael Potthoff 2 — 1 Institut für<br />
Theoretische Physik und Computational Physics, Technische Universität<br />
Graz, Petersgasse 16, A-8010 Graz, Austria — 2 Institut für Theoretische<br />
Physik und Astrophysik, Universität Würzburg, Am Hubland, D-97074<br />
Würzburg, Germany<br />
We present an extension of the recently proposed variational cluster<br />
perturbation theory to extended Hubbard models at half filling with<br />
repulsive nearest neighbor interaction. The method takes into account<br />
short-range correlations exactly by the exact treatment of clusters of finite<br />
size via exact diagonalization, whereas long-range order beyond the<br />
size of the clusters is treated on a mean-field level. We show that for one<br />
dimension results known from Quantum Monte Carlo and Density Matrix<br />
Renormalization Group can be reproduced with very good accuracy.<br />
Moreover we apply the method to the two-dimensional extended Hubbard<br />
model on a square lattice. Different from one dimension, we find a first order<br />
phase transition between spin density wave phase and charge density<br />
wave phase down to onsite interaction U = 3t. In addition, the singleparticle<br />
spectral function is calculated for both the one-dimensional and<br />
the two-dimensional system.<br />
TT 24.6 Mi 14:30 Poster A<br />
Influence of long-range Coulomb interaction and on-site<br />
Hubbard repulsion on the formation of d-wave Copper-pairing<br />
in high-Tc cuprates — •Dirk Manske 1 , Ernst Pashitskii 2 ,<br />
Vsevolod Pentegov 2 , and Ilya Eremin 1 — 1 Institut für Theoretische<br />
Physik, Freie Universität Berlin, Arnimallee 14, D-14195 Berlin<br />
— 2 Institute of Physics NAS of Ukraine, 46 Nauki str., Kiev, 03028,<br />
Ukraine<br />
We develop a diagram technique for the self-consistent treatment of<br />
the long-range Coulomb interaction and on-site Hubbard repulsion in<br />
the normal and superconducting state of high-Tc cuprates. The resultant<br />
analytical expression for the screened matrix elements taking into<br />
account long-range and on-site repulsion has been derived. In particular,<br />
it accounts for processes with and without spin-flip due to an exchange<br />
of spin and charge density fluctuations. Furthermore, we derive the expressions<br />
for the normal and anomalous self-energy parts near the superconducting<br />
transition temperature Tc that takes into account the vertex<br />
corrections including crossing diagrams. The contribution of the crossing<br />
parts is taken within the ladder approximation (similar to Fluctuations<br />
Exchange approximation) where the role of Hubbard on-site interaction<br />
is replaced by the Coulomb matrix element with a spin-flip averaged<br />
over the momentum. Finally, the developed scheme allows to analyze<br />
the formation of d-wave superconductivity and its stability in presence<br />
of the long-range Coulomb repulsion within a self-consistent anisotropic<br />
Eliashberg-like approach.<br />
TT 24.7 Mi 14:30 Poster A<br />
Electronic structure of quasi-one-dimensional metals: Theory vs<br />
Experiment — •Holger Benthien 1 , Eric Jeckelmann 2 , Florian<br />
Gebhard 1 , Michael Sing 3 , and Ralph Claessen 3 — 1 Fachbereich<br />
Physik, Universität Marburg, 35032 Marburg — 2 Institut für Physik,<br />
Universität Mainz, 55099 Mainz — 3 Experimental Physik II, Universität<br />
Augsburg, 86135 Augsburg<br />
We compare theoretical and experimental results for the electronic<br />
structure of quasi-one-dimensional correlated metals. On the one hand<br />
the one-particle Green’s function is calculated numerically in the onedimensional<br />
Hubbard model away from half filling using the dynamical<br />
density-matrix renormalization group method [1]. On the other hand the<br />
angle-resolved photoemission spectrum has been measured in the quasione-dimensional<br />
organic charge transfer salt TTF-TCNQ [2]. We show<br />
that the experimental spectrum at intermediate to high energy (up to<br />
about 1eV) can be explained consistently in the framework of the onedimensional<br />
Hubbard model. In particular, our results show clear evi-<br />
dence for spin-charge separation in the excitation spectrum (and thus for<br />
a non-Fermi liquid) up to the energy scale of the bandwidth.<br />
[1] E. Jeckelmann, Phys. Rev. B 66, 045114 (2002).<br />
[2] R. Claessen et al., Phys. Rev. Lett. 88, 096402 (2002).<br />
TT 24.8 Mi 14:30 Poster A<br />
Thermodynamic properties of ferromagnetic mixed-spin chain<br />
systems — •Noboru Fukushima 1 , Andreas Honecker 1 , Stefan<br />
Wessel 2 , and Wolfram Brenig 1 — 1 Institut für Theoretische Physik,<br />
Technische Universität Braunschweig, Germany — 2 Theoretische Physik,<br />
ETH Zürich, Switzerland<br />
Using a combination of high-temperature series expansion, exact diagonalization<br />
and quantum Monte Carlo, we perform a complementary<br />
analysis of the thermodynamic properties of one-dimensional mixed-spin<br />
systems with alternating magnetic moments. In particular, we focus on<br />
the difference between ferromagnetic (FM) and antiferromagnetic (AFM)<br />
exchange. Not only the peak structure of the specific heat is more pronounced<br />
in the FM case, but also the number of the peaks appears different.<br />
Namely, the FM case seems to have some additional energy scale(s).<br />
The origin of these differences will be discussed. In addition, the impact<br />
of interchain exchange will be also investigated.<br />
TT 24.9 Mi 14:30 Poster A<br />
Scaling of the conductance in interacting quantum wires —<br />
•Tilman Enss 1 , Sabine Andergassen 1 , Volker Meden 2 , Walter<br />
Metzner 1 , Ulrich Schollwöck 3 , and Kurt Schönhammer 2<br />
— 1 Max-Planck-Institut für Festkörperforschung, D-70569 Stuttgart<br />
— 2 Institut für Theoretische Physik, Universität Göttingen, D-37073<br />
Göttingen — 3 Sektion Physik, Universität München, Theresienstr. 37,<br />
D-80333 München<br />
The conductance through an interacting nanowire containing impurities<br />
and coupled to non-interacting leads is studied at zero and finite temperature.<br />
Our functional RG method starts from the microscopical model<br />
and arrives at an effective low-energy model correctly showing Luttinger<br />
liquid behavior. For a single impurity we observe one-parameter scaling<br />
of the conductance. Using several impurities, we study resonances of the<br />
conductance and temperature-dependent transport through a quantum<br />
dot.<br />
TT 24.10 Mi 14:30 Poster A<br />
Functional RG for Luttinger liquids with impurities — •Sabine<br />
Andergassen 1 , Tilman Enss 1 , Volker Meden 2 , Walter Metzner<br />
1 , Ulrich Schollwöck 3 , and Kurt Schönhammer 2 — 1 Max-<br />
Planck-Institut für Festkörperforschung, D-70569 Stuttgart — 2 Institut<br />
für Theoretische Physik, Universität Göttingen, D-37073 Göttingen —<br />
3 Sektion Physik, Universität München, D-80333 München<br />
Using a functional RG we compute the flow of the renormalized impurity<br />
potential for a single impurity in a Luttinger liquid over the entire<br />
energy range from the microscopic scale of a lattice-fermion model<br />
down to the low-energy limit. The non-perturbative method provides a<br />
complete real-space picture of the effective impurity potential. Further<br />
developments of the functional RG approach including 2-particle vertex<br />
renormalization considerably improve the quantitative accuracy of the<br />
results in particular at moderate interaction strenghts, which are compared<br />
to exact DMRG results. Focusing on the spectral properties of the<br />
single-particle excitations near an impurity or boundary and on the density<br />
profile, we confirm the universality of the open chain fixed point, but<br />
it turns out that very large systems are required to reach the asymptotic<br />
regime for realistic choices of the impurity and interaction parameters.<br />
TT 24.11 Mi 14:30 Poster A<br />
Coexistence of s-wave Superconductivity and Antiferromagnetism<br />
— •Martin Feldbacher 1 , Fakher Assaad 2 , Frederic<br />
Hébert 3 , and George Batrouni 3 — 1 Max-Planck-Institut für<br />
Festkörperforschung, Heisenbergstraße 1, D-70569 Stuttgart —<br />
2 Universität Würzburg, Institut für Theoretische Physik I, Am Hubland,<br />
97074 Würzburg — 3 Institut Non-Linéaire de Nice, Université de<br />
Nice-Sophia Antipolis, France<br />
We study the phase diagram of a new model that exhibits a first order<br />
transition between s-wave superconducting and antiferromagnetic phases.<br />
The model, a generalized Hubbard model augmented with competing<br />
spin-spin and pair-pair interactions, was investigated using the projector<br />
Quantum Monte Carlo method. Upon varying the Hubbard U from<br />
attractive to repulsive we find a first order phase transition between superconducting<br />
and antiferromagnetic states. Phys. Rev. Lett., 91:056401,