07.12.2012 Views

Sessions - DPG-Tagungen

Sessions - DPG-Tagungen

Sessions - DPG-Tagungen

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

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.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!