Monday, March 11, 2002 - DPG-Tagungen
Monday, March 11, 2002 - DPG-Tagungen
Monday, March 11, 2002 - DPG-Tagungen
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Nuclear Physics Tuesday<br />
HK 16.3 Tue 17:30 A<br />
Spectral Function of Quarks in Quark Matter — •Frank<br />
Frömel, Stefan Leupold, and Ulrich Mosel — Institut für<br />
Theoretische Physik, Universität Gießen, Germany<br />
We investigate the spectral function of light quarks in infinite quark<br />
matter using a simple albeit self-consistent model. Relations between<br />
correlation functions and collision rates are used to calculate the spectral<br />
function in an iterative process. Similar calculations have already<br />
been performed for nucleons in nuclear matter [1]. It was found there<br />
that this approach reproduces the results of many-body theory using a<br />
pointlike nucleon interaction with constant scattering amplitude. In our<br />
calculations the interactions between the quarks are described by the<br />
SU(2) Nambu–Jona-Lasinio model. We apply this method to calculate<br />
the quark spectral function at zero temperature and finite chemical potential.<br />
Work supported by DFG.<br />
[1] J. Lehr, H. Lenske, S. Leupold, U. Mosel, nucl-th/0108008<br />
HK 16.4 Tue 17:45 A<br />
Chiral symmetry restoration and the Z3 sectors of QCD —<br />
•Wolfgang Söldner, Christof Gattringer, P.E.L. Rakow,<br />
and Andreas Schäfer — Institut für Theoretische Physik, Universität<br />
Regensburg, D-93040 Regensburg, Germany<br />
Quenched SU(3) lattice gauge theory shows three phase transitions,<br />
namely the chiral, deconfinement and Z3 phase transition. Knowing<br />
whether or not the chiral and deconfinement phase transition occure at<br />
the same temperature for all Z3 sectors could be crucial to understand the<br />
underlying microscopic dynamics. We find that the spectral gap opens<br />
up at the same critical temperature in all Z3 sectors in contrast to earlier<br />
claims in the literature.<br />
HK 16.5 Tue 18:00 A<br />
Thermal QCD on the Lattice: Quasiparticles And Confinement<br />
— •Roland A. Schneider 1 and Wolfram Weise 1,2 — 1 Physik-<br />
Department, Technische Universität München, Garching, Germany —<br />
2 ECT*, Villazzano (Trento), Italy<br />
We propose a novel quasiparticle interpretation of the equation of state<br />
of deconfined QCD at finite temperature. Using appropriate thermal<br />
masses, we introduce a phenomenological parametrization of the onset<br />
HK17 Nuclear Physics / Spectroscopy II<br />
of confinement in the vicinity of the predicted phase transition. Lattice<br />
results of the energy density, the pressure and the interaction measure of<br />
pure SU(3) gauge theory are excellently reproduced. We find a relationship<br />
between the thermal energy density of the Yang-Mills vacuum and<br />
the chromomagnetic condensate 〈B 2 〉T. Finally, an extension to QCD<br />
with dynamical quarks is discussed. Good agreement with lattice data<br />
for 2, 2+1 and 3 flavour QCD is obtained. We also present the QCD<br />
equation of state for realistic quark masses. Applications to dilepton<br />
production in heavy-ion collisions are outlined. Published in Phys. Rev.<br />
C64 (2001) 055201.<br />
Work supported in part by BMBF and GSI.<br />
HK 16.6 Tue 18:15 A<br />
Kaons in nuclear matter — •Thomas Roth, Michael Buballa,<br />
and Jochen Wambach — Institut f. Kernphysik, TU Darmstadt<br />
We investigate the modification of Kaons in isospin symmetric and<br />
non symmetric nuclear matter. Using the leading s-wave couplings of<br />
the SU(3) chiral meson-baryon Lagrangian we solve the coupled channel<br />
Kaon-nucleon scattering equation selfconsistently.<br />
We obtain a description of the in medium properties of the Kaonnucleon<br />
scattering amplitude dominated by the Λ(1405) resonance. The<br />
in-medium Kaon propagator is calculated for different densities and different<br />
proton-neutron mixtures.<br />
While the Λ(1405) resonance is little affected by increasing density, we<br />
find that the Kaon mass experiences a strong downward shift. This will<br />
be important for the concept of Kaon condensation in neutron stars.<br />
HK 16.7 Tue 18:30 A<br />
Alpha Cluster Condensation in 12 Cand 16 O — •G. Röpke 1 , A.<br />
Tohsaki 2 , H. Horiuchi 3 ,andP. Schuck 4 — 1 FB Physik, Universität<br />
Rostock, D-18051 Rostock, Germany — 2 Department of Fine Materials<br />
Engineering, Shinshu University, Ueda 386-8567, Japan — 3 Department<br />
of Physics, Kyoto University, Kyoto 606-8502, Japan — 4 Institut de<br />
Physique Nucleaire, F-91406 Orsay Cedex, France<br />
Anewα-cluster wave function is proposed which is of the α-particle<br />
condensate type. Applications to 12 Cand 16 O show that states of low<br />
density close to the 3 and 4 α-particle thresholds in both nuclei are possibly<br />
of this kind. It is conjectured that all self-conjugate 4n nuclei may<br />
show similar features.<br />
Time: Tuesday 16:45–18:45 Room: B<br />
Group Report HK 17.1 Tue 16:45 B<br />
Peculiar Properties of Deformed Odd-Odd N = Z Nuclei —<br />
•Alexander Lisetskiy, N. Pietralla, K. Jessen, I. Schneider,<br />
A. Schmidt, andP. von Brentano — Institut für Kernphysik, Universität<br />
zu Köln, D-50937 Köln, Germany<br />
The near degeneracy of the states with total isospin quantum numbers<br />
T =0andT = 1 in odd-odd N=Z nuclei and very strong magnetic<br />
dipole (M1) transitions between them [1,2] are among the most interesting<br />
phenomena observed in N = Z nuclei. Furthermore the nuclei<br />
along the N = Z line offer a possibility to estimate the isospin mixing<br />
in the low-lying states from electromagnetic transition strengths. In the<br />
present work we analyze recent data and theoretical results on the structure<br />
of the odd-odd N=Z nuclei 46 V, 50 Mn, and 54 Co [1-4]. New data in<br />
combination either with the full pf-shell model or with collective rotorplus-quasideuteron<br />
model results help to establish systematic regularities<br />
for isovector M1 transitions, to reveal collective band structures in deformed<br />
odd-odd N = Z nuclei 46 Vand 50 Mn, and to estimate the small<br />
isospin mixing (0.4 %) between low-lying states with T =1andT =0<br />
in the odd-odd N = Z nucleus 54 Co.<br />
[1] A. F. Lisetskiy et al., Phys. Rev.C60, 064310 (1999).<br />
[2] A. F. Lisetskiy et al., Phys. Lett. B 512, 290 (2001).<br />
[3] I. Schneider et al., Phys.Rev.C61, 044312 (2000).<br />
[4] N. Pietralla et al., Phys. Rev.C65, in press (<strong>2002</strong>).<br />
Group Report HK 17.2 Tue 17:15 B<br />
High-accuracy mass measurements on N = Z nuclei using<br />
ISOLTRAP — •Frank Herfurth 1 , F. Ames 2 , G. Audi 3 , D.<br />
Beck 4 , K. Blaum 4 , G. Bollen 5 , A. Kellerbauer 1 , H.-J. Kluge 4 ,<br />
D. Lunney 3 , R.B. Moore 6 , D. Rodrígez 4 , E. Sauvan 1 , C.<br />
Scheidenberger 4 , S.Schwarz 5 , G. Sikler 4 , C. Weber 4 ,andthe<br />
ISOLDE-Collaboration 1 — 1 CERN, Geneva — 2 LMU, Munich<br />
— 3 CSNSM, Orsay — 4 GSI, Darmstadt — 5 NSCL, East Lansing —<br />
6 McGill Univ., Montreal<br />
ISOLTRAP is a Penning trap mass spectrometer installed at the online<br />
mass separator ISOLDE at CERN/Geneva. It serves for highaccuracy<br />
mass measurements of radioactive nuclides by determining their<br />
cyclotron frequency. After high-accuracy mass measurements on 74 Rb,<br />
74 Kr and 34 Ar, the mass of 32 Ar was measured recently. A relative uncertainty<br />
below 10 −7 was reached despite the short half-life of only 98 ms.<br />
This mass value is needed in the context of the search for scalar contributions<br />
to the standard model of weak interactions [1]. The experimental<br />
QEC value for the 32 Ar superallowed β decay has now the required uncertainty<br />
of only a few keV. 72 Kr is one of the two waiting point nuclei that<br />
define the speed of the astrophysical rp-process beyond A = 64. Among<br />
other things, its mass is an important input for the correct understanding<br />
and modeling of the rp-process in this region. The mass of 72 Kr was<br />
measured with a relative uncertainty of about 10 −7 .<br />
[1]E.G.Adelbergeret al., Phys. Rev. Lett. 83, 1299 and 3101 (1999)<br />
.