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 />
the hydrogen jet investigations will be presented.<br />
HK 14.31 Tue 10:30 Foyer Chemie<br />
Beam Properties of the ANKE Atomic Beam Source —<br />
•Alexandre Vassiliev1 , Reinhard Emmerich2 , Ralf Engels2 ,<br />
Vladimir Koptev1 , Peter Kravtsov1 , Jürgen Ley2 , Bernd<br />
Lorentz3 , Stefan Lorenz4 , Maxim Mikirtytchiants1,3 , Mikhail<br />
Nekipelov1,3 , Hans Paetz gen. Schieck2 , Frank Rathmann3 ,<br />
Hellmut Seyfarth3 , Erhard Steffens4 , and Hans Ströher3 — 1High Energy Physics Department, Petersburg Nuclear Physics<br />
Institute, 188300 Gatchina, Russia — 2Institut für Kernphysik,<br />
Universität zu Köln, 50937 Köln, Germany — 3Institut für Kernphysik,<br />
Forschungszentrum Jülich, 52425 Jülich, Germany — 4Physikalisches Institut II, Friedrich-Alexander Universität, 91058 Erlangen, Germany<br />
The polarized atomic beam source (ABS) will be utilized to feed the<br />
storage-cell gas target in future experiments at the magnetic spectrometer<br />
ANKE. The ABSproduces an intensity of (6.9 ± 0.3) · 1016 hydrogen<br />
atoms/s in two hyperfine substates, measured with a compression tube<br />
having the dimensions of the feeding tube of the storage-cell and installed<br />
at its position. For future polarization studies and experiments<br />
with polarized internal gas targets a Lamb-shift polarimeter, built at<br />
the University of Cologne, has been installed at the ABS. First measurements<br />
of the nuclear polarization of the atomic hydrogen beam yield<br />
Pz =0.889 ± 0.009. In addition, measurements of the degree of dissociation<br />
and of the beam profile at the position of the storage cell feeding<br />
tube will be discussed.<br />
HK 14.32 Tue 10:30 Foyer Chemie<br />
Calibration of a Compton polarimeter in a wide energy range∗ — C. Hutter1 , •D. Galaviz1 , K. Sonnabend1 , T. Hartmann1 ,<br />
P. Mohr1 , W. Rochow2 , K. Vogt1 , S . Volz1 , and A. Zilges1 — 1Institut für Kernphysik, Technische Universität Darmstadt, Schlossgartenstraße<br />
9, D-64289 Darmstadt — 2Physikalisches Institut, Universität<br />
Tübingen, Auf der Morgenstelle 14, D-72076 Tübingen<br />
A fourfold segmented High Purity Germanium detector can be used<br />
as Compton-polarimeter [1] in order to derive parities from photon scattering<br />
experiments. In order to calibrate the analyzing power of the<br />
polarimeter, (p, pγ), (p, αγ), and (α, γ) reactions have been studied in<br />
detail.<br />
We present a complete set of results up to a γ energy of 10 MeV.<br />
[1] B. Schlitt et al., Nucl. Instr. and Meth. in Phys. Res. A337 (1994)<br />
416<br />
∗ supported by DFG (Zi 510/2-1 und FOR 272/2-1)<br />
HK 14.33 Tue 10:30 Foyer Chemie<br />
Ergebnisse der Streukorrektur für die PET bei der Schwerionentherapie<br />
— •Falk Pönisch und Wolfgang Enghardt —<br />
Forschungszentrum Rossendorf e.V., Postfach 510<strong>11</strong>9, 01314 Dresden<br />
Die Behandlung von Tumourpatienten mit 12 C-IonenwirdanderGSI<br />
Darmstadt seit Dezember 1997 durchgeführt. Bei der Dosisapplikation<br />
entstehen durch Wechselwirkung des Therapiestrahls mit dem bestrahlten<br />
Gewebe β + -emittierende Nuklide. Ihre räumliche Verteilung kann<br />
online mit dem am Strahl befindlichen Doppelkopf PET Scanner nachgewiesen<br />
werden. Voraussetzung für eine retrospektive Kontrolle der Dosislokalisation<br />
ist die Rekonstruktion der Radioaktivitätsverteilung aus den<br />
Messdaten mit Hilfe eines Maximum Likelihood Expectation Maximization<br />
(MLEM) Algorithmus. Die Comptonstreuung der Annihilationsphotonen<br />
im Gewebe des Patienten beeinträchtigt die Abbildungstreue der<br />
rekonstruierten Verteilung erheblich; deshalb sind die Messdaten dagegen<br />
zu korrigieren. Die vom Strahlentherapeuten verordnete Dosis bestimmt<br />
die Zählstatistik der PET-Studien. Die Zahl der registrierten Ereignisse<br />
liegt 2 bis 3 Grössenordnungen unter der in der Nuklearmedizin üblichen.<br />
Deswegen sind die dort ausgearbeiteten Verfahren der Streukorrektur<br />
auf PET bei der Schwerionentherapie nicht anwendbar und so wurde ein<br />
Verfahren der Streukorrektur in den MLEM-Rekonstruktionsalgorithmus<br />
integriert. Anhand der Rekonstruktionen von Phantom- und Patientenmessungen<br />
konnte die Richtigkeit der Methode bestätigt werden.<br />
HK 14.34 Tue 10:30 Foyer Chemie<br />
BunchlengthmeasurementsatELBE— •Pavel Evtushenko,<br />
Ulf Lehnert, Peter Michel, and Jochen Teichert —<br />
Forschungszentrum Rossendorf (FZR),Institut fuer Kern und Hadronenphysik,Postfach<br />
510<strong>11</strong>9,01314 Dresden<br />
Last year the first ELBE accelerating module was commissioned. During<br />
the commissioning the electron beam parameters such as transverse<br />
emittance, energy spread and bunch length were measured. Each of them<br />
was studied at different bunch charges as a function of RF field phase<br />
in the first accelerating cavity. Especially for an accelerator like ELBE,<br />
which is intended to be a driver for free electron laser (FEL), bunch length<br />
measurement in picosecond range becomes very important and impose<br />
some challenge. Coherent transition radiation (CTR) technique was used<br />
to measure bunch length. This technique uses the Martin-Puplett interferometer<br />
to measure the autocorrelation of the CTR pulse yielding a<br />
minimum 2 ps RMSbunch length at 77pC bunch charge. Short description<br />
of the method, experimental setup, data evaluation procedure and<br />
results of the measurements will be presented.<br />
HK 14.35 Tue 10:30 Foyer Chemie<br />
Investigation of light spots and related field emission at the<br />
S–DALINAC ⋆ — •M. Gopych, W. Beinhauer, M. Brunken, H.-<br />
D. Gräf, T. Hartmann, M. Hertling, S.Kostial, U. Laier, A.<br />
Lenhardt, M. Platz, A. Richter, B. Schweizer, A. Stascheck,<br />
O. Titze, andS.Watzlawik—Inst.für Kernphysik, TU Darmstadt,<br />
Schlossgartenstr. 9, 64289 Darmstadt<br />
Above certain field thresholds spots of light associated with field emission<br />
have been observed on the surface of an RF niobium superconducting<br />
cavity at the S–DALINAC. The spectrum of the optical radiation has<br />
been measured by an spectrometer set up on axis at the beam line exit<br />
of the accelerator. It shows a sharp peak at 693 nm and three small ones<br />
at about 670 nm, 705 nm, and 714 nm. Measurements of field dependence<br />
and intensity of the light spots revealed a behaviour similar to the<br />
electroluminescence phenomenon. Additional results of measurements<br />
aiming at the investigation of the emission of light and related field emission<br />
performed at the superconducting cavities will be presented.<br />
⋆ Supported by the DFG (FOR 272/2-1 and GRK 410/2)<br />
HK 14.36 Tue 10:30 Foyer Chemie<br />
Trigger and Readout for the Auger-Fluorescence telescopes —<br />
•Andreas Kopmann, Hermann-Josef Mathes, Hartmut Gemmeke,<br />
Matthias Kleifges, Alexandre Menshikov, and Denis<br />
Tcherniakhovski — Institut f”ur Prozessdatenverarbeitung und Elektronik,<br />
Forschungszentrum Karlsruhe<br />
The Pierre Auger Collaboration started with the construction of the<br />
first hybrid detector in Argentina. In the final state this experiment will<br />
consist of a large array of Cerenkov water detectors and 30 fluorescence<br />
telescopes to observe fluorescence light of EAS(Extensive air shower)<br />
with energies above 10 18 eV. Each telescope will be equipped with an<br />
independent trigger and readout system. The combination of fast hardware<br />
based pattern recognition and special software algorithms provide<br />
a trigger rate of a few events per hour.<br />
Since October 2001 two of this camera systems are operational. They<br />
demonstrate the power of the realized concept. The actual implemented<br />
trigger algorithms and their efficiency as well as the first data are presented.<br />
HK 14.37 Tue 10:30 Foyer Chemie<br />
ROOT-based off-line and on-line analysis of COSY-TOF data ∗<br />
— •Martin Schulte-Wissermann and Leonhard Karsch for the<br />
COSY-TOF collaboration — Institut für Kern- und Teilchenphysik, TU<br />
Dresden, Germany<br />
The COSY-TOF spectrometer is used to study proton-proton collisions<br />
with up to 2.5 GeV kinetic energy. During an experiment which<br />
lasts typically several weeks data in the order of 100 GB are stored on<br />
tape. Due to the modular setup of the detector, which is optimized for<br />
each individual experiment, the data analysis software has to be adapted<br />
accordingly.<br />
Using ROOT as the fundamental framework, we have developed a strategy<br />
(set of rules) how to efficiently combine the contributions of all collaborators<br />
involved in the data analysis. We provide interfaces, data<br />
containers, and function libraries which are easy to use, robust, and well<br />
documented. The application of these tools in the analysis of COSY-<br />
TOF data will be demonstrated.<br />
The usefullness of the whole concept in the on-line supervision and calibration<br />
was shown during a recent run. ∗ Supported by BMBF and FZJ.