Sessions - DPG-Tagungen
Sessions - DPG-Tagungen
Sessions - DPG-Tagungen
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Nuclear Physics Tuesday<br />
The linear sigma-model with quarks provides a valid description of<br />
QCD on a scale below approximately 1.3 GeV. It is well suited to describe<br />
the physics of the chiral symmetric phase at the UV scale, as well<br />
as he physics at low energies characterized by chiral symmetry breaking.<br />
Starting with the theory given at the UV scale, in the renormalization<br />
group approach infinitesimal shells of large momentum modes are<br />
integrated out and the couplings of the theory are renormalized. In this<br />
way, an effective low energy theory is obtained by evolving the couplings<br />
towards small momentum scales.<br />
In order to enable a comparison with results from lattice QCD, we<br />
consider a renormalization group treatment of the linear sigma model in<br />
a finite Euclidean volume. The renormalization group flow equations are<br />
derived and solved numerically. Explicit breaking of the chiral symmetry<br />
is considered through the introduction of a finite quark mass.<br />
We obtain results for the volume dependence of the chiral condensate.<br />
In accordance with the results obtained from finite volume partition<br />
functions, the mesonic zero modes are important for the evolution<br />
of the couplings at low renormalization scales.<br />
HK 20.4 Tue 16:45 E<br />
RG analysis of the quark-meson model at finite temperature<br />
and density — •Bernd-Jochen Schaefer and Jochen Wambach<br />
— IKP, Schlossgartenstrasse 9,D-64289 Darmstadt<br />
Renormalization group equations obtained by means of a proper-time<br />
regulator are used in order to analyze the chiral symmetry restoration<br />
at finite temperature and density in the two flavor quark-meson model.<br />
Results for the Nf = 2 QCD phase diagram are presented and compared<br />
with those coming from lattice simulations.<br />
HK 20.5 Tue 17:00 E<br />
Properties of two- and three-quark states in hot and dense matter<br />
— •S. Mattiello 1 , M. Beyer 1 , S. Strauss 1 , T. Frederico 2 ,<br />
and H.J. Weber 3 — 1 FB Physik, U Rostock, Germany — 2 CTA, Sao<br />
Jose dos Campos, Brazil — 3 U of Virginia, Charlottesville, USA<br />
In the framework of the light front field theory at finite temperature<br />
and density we investigate the formation of two- and three-body bound<br />
states in quark matter. This approach leads to the dominant medium<br />
effects, i.e. the Pauli blocking and the self energy corrections. Utilizing<br />
the Nambu-Jona-Lasinio model on the light front we study the chiral<br />
restauration and the dependence of pionic properties (mass and decay<br />
costante) on the temperature and the chemical potential. The threequark<br />
dynamics is investigated using a scalar zero-range interaction and<br />
the results for the dependence on the medium of the three-body mass<br />
are presented. The dissociation of the three-quark state as well as the<br />
critical temperature of the color-superconducting phase are investigated.<br />
Acknowledgement: Work supported by Deutsche Forschungsgemeinschaft.<br />
HK 20.6 Tue 17:15 E<br />
Quasiparticle Description of Hot QCD at Finite Quark Chemical<br />
Potential (∗) — •Michael Thaler 1 , Roland Schneider 1,2 , and<br />
Wolfram Weise 1,2 — 1 Physik Department Technische Universität<br />
München — 2 ECT ∗ , Villa Tambosi, Trento, Italy<br />
We study the extension of a phenomenologically successful quasiparticle<br />
model that describes lattice results of the equation of state of the<br />
deconfined phase of QCD for Tc ≤ T ∼ < 4Tc, to finite quark chemical<br />
potential µ. The phase boundary line Tc(µ), the pressure difference<br />
∆p(T, µ) = (p(T, µ) − p(T, µ = 0))/T 4 and the quark number density<br />
nq(T, µ)/T 3 are calculated and compared to recent lattice results. Good<br />
agreement is found up to quark chemical potentials of order µ ∼ Tc. (∗)<br />
Work supported in part by BMBF and GSI.<br />
HK 20.7 Tue 17:30 E<br />
The effect of quark off-shellness in high energy processes —<br />
•Olena Linnyk, Stefan Leupold, and Ulrich Mosel — Institut<br />
für Theoretische Physik, Universität Giessen, 35392 Giessen, Germany<br />
We study the quark and gluon structure of hadrons going beyond the<br />
well-known picture of collinear non-interacting partons. Calculated are<br />
the effects of an initial quark off-shellness in several high energy processes.<br />
The interaction of the partons missed in the standard perturbative consideration<br />
is taken into account in the spectral functions of the quarks,<br />
and using a generalized factorization. The intrinsic motion of the partons<br />
is consistently treated as well. The quark off-shellness turns out to<br />
be important in the description of semi-exclusive observables such as the<br />
triple differential Drell-Yan cross section. Recent data of the Fermilab<br />
experiment E866 on continuum dimuon production are analyzed and the<br />
width of the quark spectral function in the proton is found to be approximately<br />
150 MeV. The dependence of the width on the hard scale is<br />
investigated. The results of our calculations reveal the important role of<br />
the initial quark virtuality in high energy processes.<br />
Work supported by the European graduate school Giessen–Copenhagen.<br />
HK 20.8 Tue 17:45 E<br />
Stable gapless color superconducting phases of dense quark<br />
matter — •Igor Shovkovy — Institute for Theoretical Physics, Johann<br />
Wolfgang Goethe University, 60325 Frankfurt am Main<br />
I review the zero and finite temperature properties of the recently proposed<br />
gapless color superconducting phase of neutral dense quark matter<br />
in β-equilibrium. This is a stable phase of quark matter that could exist<br />
inside cores of compact stars.<br />
HK 20.9 Tue 18:00 E<br />
ρ −ω splitting and mixing in nuclear matter — •Sven Zschocke<br />
and Burkhard Kämpfer — Forschungszentrum Rossendorf e.V., Institut<br />
für Kern- und Hadronenphysik, D-01314 Dresden,Postfach 51 01<br />
19<br />
We investigate mass splitting and mixing effect of ρ and ω mesons<br />
in nuclear matter within the QCD sum rule approach in zero-width approximation.<br />
In matter, ρ and ω differ only by a scalar flavour mixed<br />
condensate and a twist-4 four-quark condensate as long as one is restricted<br />
to dimension-6 operators. In our sum rule analysis we have<br />
taken into account both condensates and investigate the impact of the<br />
poorly known four-quark condensate. Both effects, mixing and splitting,<br />
are much stronger in a nuclear medium than in vacuum. This triggers<br />
the hope to verify this in-medium effects with experiments like HADES<br />
at GSI.<br />
HK 20.10 Tue 18:15 E<br />
Suppression of high transverse momentum particles at RHIC by<br />
(pre–)hadronic FSI — •Kai Gallmeister, Wolfgang Cassing,<br />
and Carsten Greiner* — Institut für Theoretische Physik, Universität<br />
Giessen, 35392 Giessen, Germany (*present address: Institut für<br />
Theoretische Physik, Universität Frankfurt, 60054 Frankfurt am Main,<br />
Germany)<br />
We investigate transverse hadron spectra from proton+proton,<br />
deuteron+Au and Au+Au collisions at √ s = 200 GeV within the<br />
Hadron–String–Dynamics (HSD) approach which is based on quark, diquark,<br />
string and hadronic degrees of freedom, combined with Pythia<br />
calculations for high p⊥ spectra. The comparison to experimental data<br />
from RHIC shows that pre–hadronic effects of the leading hadrons can<br />
be responsible for both the hardening of the spectra for low transverse<br />
momenta as well as the suppression of high p⊥ hadrons. The interactions<br />
of formed, non–leading hadrons are found to be more or less negligible<br />
for p⊥ ≥ 8 GeV/c and cannot be responsible for the large suppression<br />
seen experimentally, but they have some importance for lower p⊥ values.<br />
These findings are in nice agreement with the hadron attenuation<br />
observed in virtual photon induced reactions on nuclei at HERMES, cf.<br />
Thomas Falter’s talk.<br />
Work supported by BMBF.