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Monday, March 11, 2002 - DPG-Tagungen

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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-

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