Monday, March 11, 2002 - DPG-Tagungen
Monday, March 11, 2002 - DPG-Tagungen
Monday, March 11, 2002 - DPG-Tagungen
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
Nuclear Physics Thursday<br />
(LHC), where rapidity densities of charged particles up to dN/dy = 8000<br />
are anticipated in collisions of Pb nuclei at √ s =5.5 ATeV.<br />
Along with a general overview of the detector, results from extensive<br />
in-beam tests with regard to transition radiation yield, pion rejection,<br />
and tracking performance will be presented. Using the experimental data<br />
the performance of the fast electron trigger has been simulated. Finally,<br />
the anticipated performance of the trigger for quarkonia measurements<br />
at central rapidity will be demonstrated.<br />
HK 41.3 Thu 14:45 E<br />
Investigation of the event anisotropy with the CERES/NA45<br />
experiment — •Jana Slivova and Jovan Milosevic for the<br />
CERES/NA45 collaboration — Physikalisches Institut der Universität<br />
Heidelberg, Philosophenweg 12, 69120 Heidelberg<br />
Using the data obtained at the CERES/NA45 experiment the elliptic<br />
event anisotropy was studied in Pb+Au collisions at 40, 80, and 158<br />
AGeV/c. This anisotropy is quantified by the second Fourier coefficient<br />
(v2). Results are obtained both for identified pions and for charged particles.<br />
We will compare values of v2 obtained using different methods<br />
- standard flow analysis with respect to the reaction plane, two-particle<br />
correlations, and preliminary results from the recently introduced method<br />
of cumulants (Phys. Rev. C 63, 054906 (2001)).<br />
HK 41.4 Thu 15:00 E<br />
Charge fluctuations in nuclear collisions: experimental results<br />
and model studies. — •Jacek Zaranek 1 , P. Dinkelaker 1 , L.<br />
Betev 1 , C. Blume 2 , R. Bramm 1 , P. Buncic 1 , M. Ga´zdzicki 1 ,<br />
T. Kollegger 1 , I. Kraus 2 , A. Mischke 2 , R. Renfordt 1 , A.<br />
Sendoval 2 , R. Stock 1 , H. Ströbele 1 , D. Vranic 2 ,andA. Wetzler<br />
1 for the NA49 collaboration — 1 University of Frankfurt, IKF —<br />
2 GSI, Darmstadt<br />
HK42 Instrumentation and Applications V<br />
Study of event-by-event fluctuations of electric charge in high energy<br />
nucleus-nucleus collisions may provide information on the state of matter<br />
in an early stage of the collision. They should be also sensitive to the<br />
number of resonances at chamical freez-out. Preliminary experimental<br />
data obtaind by NA49 on charge fluctuations in central Pb+Pb collisions<br />
at 40, 80 and 158 AGeV will be shown. The results will be discussed in<br />
the framework of serveral models in which the effects of global charge<br />
conservation, resonances decay kinematics and QGP formation are studied.<br />
HK 41.5 Thu 15:15 E<br />
Event-by-Event Fluctuations at 40, 80 and 158 AGeV/c in<br />
Pb+Au Collisions from CERES/NA45 — •Hiroyuki Sako and<br />
Harald Appelshäuser —GSI,Darmstadt<br />
Event-by-event fluctuations have been proposed as probes to search<br />
for the QCD critical point and deconfined phase.<br />
We present fluctuations of mean pT and charge multiplicity ratios at<br />
40, 80, and 158 AGeV/c in Pb+Au Collisions. We also compare them<br />
with other experimental data and with theoretical expectations.<br />
Time: Thursday 14:00–15:30 Room: F<br />
Group Report HK 42.1 Thu 14:00 F<br />
The AGOR facility — •S. Brandenburg, W. van Asselt, J.P.M.<br />
Beijers, H.R. Kremers, T. Nijboer, H. Post, and S . van<br />
der Veen — Kernfysisch Versneller Instituut, 9747 AA Groningen, the<br />
Netherlands<br />
The heart of the AGOR facility at the KVI is a superconducting cyclotron,<br />
constructed by a collaboration of the KVI and the IPN, Orsay,<br />
France. The facility is operational since 1997 for some 4500 hours per<br />
year. The cyclotron can accelerate both light and heavy ions (e.g. protons<br />
up to 190 MeV, lead down to 6 MeV/nucleon). It is equipped with<br />
ion sources for polarized hydrogen, light and heavy ions.<br />
The basic characteristics and performance of the facility will be described.<br />
The design issues related to the wide range of ions and energies<br />
will be discussed. Furthermore attention will be given to new developments,<br />
such as the acceleration of low-intensity triton beams.<br />
HK 42.2 Thu 14:30 F<br />
New Developments in Cryo Targets for the External COSY Experiments<br />
— •S. Abdel-Samad, M. Abdel-Bary, andK. Kilian<br />
for the COSY-TOF collaboration — Forschungszentrum Juelich<br />
For pp and pd interaction studies at COSY a very light cryo target<br />
has been developed. The target thickness in beam direction defines the<br />
interaction probability and thus the statistical precision. However all<br />
material which can be hit by particles from the reaction under study<br />
will produce secondary scattering and unwanted background. Therefore<br />
already the target thickness has to be kept short. Much more important<br />
is to keep the transversal size of the target very small and the heat conductors,<br />
mounting elements and thermal isolation as light as possible.<br />
The Juelich cryo targets have been optimized over some years in this<br />
aspect. A drastic reduction of the total mass of the target arrangement<br />
was achieved by using very thin walled, small diameter heat pipes, by<br />
using aluminum for condensers, by target cells of galvanically deposited<br />
copper and by 0.9 µm Mylar windows. Up to 2 meter long heat pipes<br />
are operational. For bubble free operation a temperature stability with<br />
< 0.2 K fluctuation has to be achieved. Details of the targets will be<br />
shown.<br />
HK 42.3 Thu 14:45 F<br />
A Silicon Tracking Telescope for Spectator Proton Detection<br />
— •A. Mussgiller 1 , G. Fiori 1 , T. Krings 1 , S. Merzliakov 2 ,<br />
D. Protic 1 , and R. Schleichert 1 for the ANKE collaboration —<br />
1 Institut für Kernphysik, Forschungszentrum Jülich — 2 Laboratory of<br />
Nuclear Problems, JINR, Dubna, Russia<br />
The identification and tracking of low energy protons enables the use of<br />
deuterons as an effective neutron target. For this purpose a self-triggering<br />
tracking telescope has been developed. The telescope consists of three<br />
layers of double-sided silicon strip detectors mounted inside the COSY<br />
vacuum. The setup allows the identification of protons from 1.5 MeVto<br />
40 MeV via the ∆E/E method and particle tracking over a wide range<br />
from 1.5 MeV protons to minimum ionizing particles. Results of the first<br />
measurements will be presented.<br />
HK 42.4 Thu 15:00 F<br />
Nuclear Polarization of Molecular Hydrogen — •F. Rathmann 1 ,<br />
J.T. Balewski 2 , J. Doskow 2 , W. Haeberli 3 , B. Lorentz 1 , H.O.<br />
Meyer 2 , P.V. Pancella 4 , R.E. Pollock 2 , B. v. Przewoski 2 ,<br />
P.A. Quin 3 , T. Rinckel 2 , Swapan K. Saha 5 , B. Schwartz 3 , T.G.<br />
Walker 3 , A. Wellinghausen 2 ,andT. Wise 3 — 1 IKP, FZJ, Jülich,<br />
Germany — 2 IUCF, Bloomington, USA — 3 Dep. of Physics, University<br />
of Wisconsin-Madison, USA — 4 Western Michigan University, Kalamazoo,<br />
USA — 5 Bose Institute, Calcutta, India<br />
We have measured the nuclear polarization of hydrogen molecules<br />
formed by recombination of polarized atomic hydrogen gas [1]. A polarized<br />
atomic hydrogen beam is incident upon a copper recombination<br />
zone and subsequently drifts into an internal target located in a straight<br />
section of the IUCF Cooler ring. The target contains an internal valve<br />
that allows us to rapidly alternate between a mostly atomic and a mostly<br />
molecular target. A comparison of the target polarization for these two<br />
states can be used to determine the fraction of the initial atom polarization<br />
that survives recombination and subsequent wall collisions in the<br />
target. That fraction was studied for temperatures between 50 K and<br />
300 K and for applied magnetic fields between 0.5 mT and 0.6 T. The<br />
target polarization was measured with a 200 MeV longitudinally polarized<br />
proton beam using the known [2] large pp elastic spin correlation<br />
coefficient Azz. The apparatus, measurement methods, results and inter-