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Monday, March 11, 2002 - DPG-Tagungen

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Nuclear Physics Thursday<br />

HK48 Instrumentation and Applications VI<br />

Time: Thursday 16:00–18:00 Room: F<br />

Group Report HK 48.1 Thu 16:00 F<br />

Investigaions of scintillation detectors for relativistic heavy ion<br />

calorimetry — •Radomira Lozeva 1,2 , Jürgen Gerl 1 , Ivan Kojouharov<br />

1 , Samit Mandal 1 ,andJuri Kopatch 1 — 1 GSI, Darmstadt,<br />

Germany — 2 Faculty of Physics, University of Sofia, Sofia, Bulgaria<br />

To gain information on the energy resolution of scintillators for heavy<br />

ion detection at high particle energy an in-beam test was performed at<br />

the Fragment Separator, FRS at GSI. Primary 197 Au beam was transported<br />

through FRSand particle identification detectors to the scintillator<br />

set-up. CsI(Tl)+PMT, CsI(Tl)+PIN diode, NaI(Tl), BGO and<br />

Plastic scintillation detectors were selected for investigation.<br />

The results of the in-beam test analysis showed satisfactory results for<br />

the CsI(Tl)+PMT scintillator. An energy resolution of 0.46% FWHM<br />

for 197 Au ions of 306 MeV/n ion energy was achieved with appropriate<br />

analysis conditions. The obtainable resolution is sufficient for further<br />

mass determination of heavy ions by calorimetry and will therefore be<br />

chosen for the fast beam RISING [1] campaign at GSI.<br />

[1] http://www-aix.gsi.de/ ∼ wolle/EB at GSI/rising.html<br />

HK 48.2 Thu 16:30 F<br />

Performance of the Pre-Shower System in the HADES Spectrometer<br />

— •Jerzy Pietraszko for the HADEScollaboration — GSI,<br />

Darmstadt<br />

The Pre–Shower detector system of the HADES spectrometer is applied<br />

to electron identification with emphasis on fast pion rejection at<br />

forward angles. The detector is operated in the self–quenching streamer<br />

mode (SQS) to simplify on-line recognition of electromagnetic showers.<br />

Stable electronics at low noise guarantee robust pattern recognition<br />

through the experimental runs. On-line analysis results delivered by<br />

dedicated pattern recognition units show perfect agreement with results<br />

derived in the off-line analysis. The performance of the detector and<br />

readout system will be presented.<br />

HK 48.3 Thu 16:45 F<br />

HADES Drift Chambers (MDC III) — •Kalliopi Kanaki,<br />

Frank Dohrmann, Rugard Dressler, Wolfgang Enghardt,<br />

Eckart Grosse, Klaus Heidel, Jochen Hutsch, Burkhard<br />

Kämpfer, Roland Kotte, Lothar Naumann, Alexandre<br />

Sadovski, Joachim Seibert, and Manfred Sobiella for the<br />

HADEScollaboration — Forschungszentrum Rossendorf, Institut für<br />

Kern- und Hadronenphysik, Dresden, Germany<br />

The starting experiments with the High Acceptance Di-Electron<br />

Spectrometer (HADES) at GSI/Darmstadt require a momentum resolution<br />

of about 1%, i.e. the determination of particle tracks with a precision<br />

better than 100 µm. The tracking is accomplished mainly by largearea<br />

Multiwire Drift Chambers. Four of the MDC’s of the third plane<br />

(MDC III), produced in the Research Centre Rossendorf, have been already<br />

installed in the HADESspectrometer. In this talk, the technical<br />

aspects of the MDC III construction, the operational characteristics, and<br />

several tests performed are discussed. We also presented simulations<br />

of the electrical field configurations and resulting drift velocity patterns<br />

which are aimed at an optimision of the chamber performance.<br />

HK 48.4 Thu 17:00 F<br />

Measurement of π 0 -induced leptons in the HADES RICH ∗ —<br />

•T. Eberl, L. Fabbietti, J. Friese, R. Gernhäuser, J. Homolka,<br />

H.-J. Körner, M. Münch, B. Sailer, andS. Winkler — Technische<br />

Universität München, James-Franck-Strasse 1,D-85748 Garching<br />

A fast Ring Imaging Cherenkov detector (RICH) is the central device<br />

of the new dilepton spectrometer HADESat GSI, Darmstadt. It serves<br />

as a hadron blind trigger device for e + e − pairs in hadron and heavy ion<br />

induced collisions at 1-2 AGeV incident energy, in which π 0 are produced<br />

abundantly.<br />

The main sources of lepton pairs with small opening angles (1-15<br />

degrees) are π 0 -Dalitz decays (π 0 → e ± γ) and photo conversion pairs<br />

(π 0 → 2γ; γ → e ± ) from the target, the C4F10 gas radiator and the VUV<br />

transparent CaF2 window. These lepton signals contribute significantly<br />

to the combinatorial background, if they are not identified properly.<br />

We report on the analysis and classification of measured lepton-induced<br />

ring patterns on the RICH photocathode from a dedicated low magnetic<br />

field measurement in correlation with data from the HADEStracking<br />

(MDC) and time-of-flight (TOF wall) subdetectors.<br />

∗ supported by BMBF (6TM970I) and GSI (TM-FR1).<br />

HK 48.5 Thu 17:15 F<br />

Charged Particle Detection with PbWO4 — •Matthias Hoek 1 ,<br />

Werner Döring 1 , Volker Hejny 2 , Herbert Löhner 3 , Volker<br />

Metag 1 , Rainer Novotny 1 , and Heinrich Wörtche 3 — 1 II.<br />

Physikalisches Institut, Universität Giessen, Germany — 2 Institut für<br />

Kernphysik, FZ-Jülich, Germany — 3 Kernfysich Versneller Instituut,<br />

Groningen, The Netherlands<br />

TheresponseofPbWO4 to high energy charged hadrons has been investigated<br />

in two test experiments at the proton beam facilities COSY,<br />

FZ-Jülich (E=1.2 GeV) and AGOR, KVI, Groningen (E=85MeV). For<br />

the first time, the energy resolution for protons and deuterons below 360<br />

MeV energy, which were stopped within 150 mm of PbWO4, has been<br />

determined to σ/E=0.97%/ √ E + 3.33%. The result is comparable to<br />

the previously deduced photon response. Energy spectra of inelastically<br />

scattered protons below 85MeV measured with pure and doped PbWO4crystals<br />

are compared to similar distributions obtained for BaF2- and<br />

CeF3-detectors. The comparison to the response of charged pions indicates<br />

a strong quenching factor (¿3) of the scintillation light for hydrogen<br />

isotopes. The obtained results document the applicability of PbWO4 in<br />

photon and particle detection at medium energies.<br />

HK 48.6 Thu 17:30 F<br />

Large-Area Glass Resistive Plate Chambers (GRPC) as Fast<br />

Timing Detector — •Zbigniew Tyminski — Gesellschaft für Schwerionenforschung,<br />

Darmstadt, Germany<br />

In the framework of the FOPI upgrade project our collaboration is<br />

planning to build another time-of-flight detector shell capable of coping<br />

with the expected multiplicity of 80-100 charged particles (central<br />

Au+Au collisions at 1.5A GeV) at time resolutions below 100 ps. A possible<br />

solution are Glass Resistive Plate Chambers [1]. We have studied<br />

several prototypes of such detectors (400 cm 2 big) with 4 gaps of 300µm<br />

between glass plates of 0.5-2 mm thickness and intermediate strip electrodes<br />

formed of 12 or 16 parallel strips (pitch ≈ 3mm) which are read<br />

out on each side. The time is obtained by mean timing of the 2 signals,<br />

their difference delivers the position along the strip; charge averaging<br />

over neighbouring strips yields the perpendicular position. We describe<br />

details of the prototypes as well as tests in which we have obtained σ ≈ 70<br />

ps at efficiencies above 95%.<br />

[1] P.Fonte et al., NIM A449(2000)295<br />

HK 48.7 Thu 17:45 F<br />

The potential of in-beam PET for proton therapy monitoring:<br />

first experimental investigation — •Katia Parodi 1 , Wolfgang<br />

Enghardt 1 ,andThomas Haberer 2 — 1 Forschungszentrum<br />

Rossendorf e.V., Postfach 510<strong>11</strong>9, 01314 Dresden — 2 Gesellschaft für<br />

Schwerionenforschung, Planckstr. 1, 64291 Darmstadt<br />

On the basis of the positive clinical impact of in-beam PET on the<br />

quality assurance of carbon ion therapy at GSI Darmstadt [1] we started<br />

to investigate the potential extension of the technique to proton therapy.<br />

This is non-trivial, since protons cannot suffer the projectile fragmentation<br />

process which leads to a pronounced maximum of the β + activity in<br />

close vicinity to the dose maximum in the carbon ion case.<br />

In our experiment three monoenergetic proton beams in the energy<br />

and intensity range of therapeutic interest were stopped in targets of<br />

PMMA (C5H8O2) placed in the centre of the field of view of the in-beam<br />

positron camera installed at the GSI heavy ion therapy facility. The β +<br />

activity signal was found to be three times larger than that induced by<br />

carbon ions at the same range and applied physical dose. The reconstructed<br />

spatial β + activity distributions were well reproduced in shape<br />

by a calculation based on experimental cross-sections and on the proton<br />

flux given by the FLUKA Monte Carlo code. Despite the weaker<br />

spatial correlation between activity and dose depth-distributions in the<br />

proton case, our experiment supports the feasibility of in-beam PET for<br />

the monitoring of proton therapy based on a comparison between measured<br />

and calculated β + activity distributions, as already implemented<br />

for carbon ion therapy.<br />

[1] W. Enghardt et al, Nucl. Phys. A 654 1047c (1999)

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