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 />
bution describes the probability to find a transversely polarized quark<br />
in a transversely polarized nucleon. The unpolarized quark density q(x),<br />
the longitudinally polarized quark density ∆q(x) and the transversity<br />
distribution δq(x) together provide a complete description of the quark<br />
and spin density distributions in leading order (twist-2).<br />
For semi-inclusively produced π + and π 0 on a hydrogen target a significant<br />
moment of sin φ is observed in the azimuthal distribution. For π −<br />
the sin φ moment is found to be small. Since 1998 HERMES is taking<br />
data with a polarized deuteron target.<br />
An investigation of the flavour dependence of the transversity distribution<br />
δq(x) will be possible with the measurement of single-spin asymmetries<br />
for different hadrons (π + , π 0 , π − and K + ) and different target<br />
nucleons.<br />
This project is supported by the German BMBF.<br />
HK 12.14 Tue 10:30 Foyer Chemie<br />
Measurement of inclusive K-meson production in B-meson decays<br />
using the BABAR detector — •Stefan Christ for the<br />
BABAR collaboration — AG Elementarteilchenphysik, Universitätsplatz<br />
3, 18051 Rostock<br />
A method to measure the K-meson spectrum from B 0 , ¯ B 0 , B + and<br />
B − decays at the BABAR detector is presented. The BABAR detector is<br />
operated at the PEP-II asymmetric B-meson factory at SLAC. B-mesons<br />
are produced in pairs from Υ(4S) decays with opposite b-quark flavour.<br />
Fully reconstructing one B-meson that decayed into a flavour tagging<br />
channel provides information about the b-quark flavour of this second<br />
B-meson. All particles not used for the reconstruction have to originate<br />
from the second B-meson. By identifying these particles the K-meson<br />
spectrum can be measured for each flavour individually. The analysis<br />
method is presented. The performance of the particle identification is<br />
determined without Monte Carlo simulation.<br />
HK 12.15 Tue 10:30 Foyer Chemie<br />
Measurement of Inclusive η Production in e + e − -Annihilation<br />
Reactions with the BABAR Experiment — •Denis Altenburg<br />
for the BABAR collaboration — TU Dresden, Institut fuer Kern- und<br />
Teilchenphysik, 01062 Dresden<br />
The η momentum spectra and multiplicities in multihadronic events<br />
from e + e − -annihilation reactions are measured using 14.3 fb −1 on the<br />
Υ(4S) resonance ( √ s ≈ 10.58 GeV) and 2.6 fb −1 off resonance data<br />
( √ s ≈ 10.54 GeV) collected with the BABAR detector. The η mesons<br />
are reconstructed using the decay mode η → γγ. The inclusive branching<br />
ratio of B mesons to η mesons B(B →ηX ) has been determined and has<br />
been found to be in reasonable agreement to the corresponding CLEO<br />
result.<br />
HK 12.16 Tue 10:30 Foyer Chemie<br />
Search for the Decay D ∗ s → Dsπ 0 and Measurement of the Partial<br />
Widths Ratio Γ(D ∗ s → Dsπ 0 )/Γ(D ∗ s → Dsγ) with BABAR —<br />
•Martin Dickopp for the BABAR collaboration — Inst. f. Kern- und<br />
Teilchenphysik, TU Dresden, 01062 Dresden<br />
The search for the isospin violating decay D ∗ s → Dsπ 0 in data accumulated<br />
with the BABAR detector located at the asymmetric e + e −<br />
storage facility PEP-II at SLAC is presented. Furthermore, the partial<br />
widths ratio Γ(D ∗ s → Dsπ 0 )/Γ(D ∗ s → Dsγ) has been measured. The<br />
result improves the precision of a measurement by CLEO in 1995.<br />
HK 12.17 Tue 10:30 Foyer Chemie<br />
Search for Eta-nucleus bound state at COSY, Juelich — B. Roy,<br />
H. Machner, •B. Roy, andH. Machner for the GEM collaboration<br />
and the GEM collaboration — Institut für Kernphysik, Forschungszentrum<br />
Jülich, Jülich, Germany<br />
In contrast to the π -nucleon interaction, the η-nucleon interaction<br />
is strong and attractive at low energies ( S-wave ). This provides an<br />
interesting possibility of the existence of the eta-nucleus bound states,<br />
and their production in near threshold η production in proton nucleus<br />
collisions. We plan to produce these η-nuclei in p+ A ZX → 3 He+ A−2<br />
Z−1Yη<br />
or p+ A Z<br />
X → d+A−1<br />
Z Xη reactions by choosing the “magic momentum”of<br />
the proton-beam and the detection angle of 3 He/d such that the η is<br />
produced with very small momentum. In order to detect the η -mesic<br />
nucleus events in the presence of large background, it would be necessary<br />
to demand a triple coincidence of 3 He and the η -mesic nucleus decay<br />
particles, namely, protons and pions. In order to tag the η -mesic nucleus<br />
through its decay products, a large acceptance plastic scintillator<br />
detector “ENSTAR” is being built in Mumbai, India. The detector fab-<br />
rication is at an advanced stage at BARC, Mumbai and will be shipped<br />
to Jülich immediately after the completion of the construction work.<br />
HK 12.18 Tue 10:30 Foyer Chemie<br />
Search for a quasi-bound 3 Heη state at the COSY-TOF spectrometer<br />
— •A. Gillitzer for the COSY-TOF collaboration — IKP,<br />
Forschungszentrum Jülich<br />
The peculiar behavior of the pd → 3 Heη cross section close to threshold<br />
has been interpreted as being the result of a quasi-bound state of the<br />
3 Heη system just below the threshold. We will study this longstanding<br />
question in a formation experiment at the COSY-TOF spectrometer, by<br />
measuring the excitation function of the reaction pd → pppπ − in the<br />
bound region of the 3 Heη system. This is a sensitive observable because<br />
the decay of a quasi-bound 3 Heη state is expected to be dominated by<br />
the ηN → πN channel with two spectator nucleons, a final state having<br />
a characteristic kinematical topology. The COSY-TOF spectrometer including<br />
the forward calorimeter is particularly well-suited for the study<br />
the of the pppπ − final state, i.e. the absorption of the η mesononthe<br />
neutron in 3 He, since the TOF spectrometer has both large acceptance<br />
for the pπ − pair and good particle identification for the pp spectator pair.<br />
The outline of the experiment will be presented, including a discussion<br />
of expected background reactions.<br />
HK 12.19 Tue 10:30 Foyer Chemie<br />
Study of η production on light nuclei — M. Ulicny 1 , H. Machner<br />
2 , •M. Ulicny 1 ,andH. Machner 2 for the GEM collaboration and<br />
the GEM collaboration — 1 University of P. J. ˇ Safárik, Koˇsice, Slovakia<br />
— 2 Institut für Kernphysik, Forschungszentrum Jülich, Jülich, Germany<br />
The production of η-mesons on light nuclei in proton induced reactions<br />
is of interest, because of the high momenta transferred in the reaction,<br />
considerably larger than in pion production. Such high momenta can not<br />
be transferred in a NN-interaction This makes the p + 6 Li → 7 Be + η<br />
reaction especially interesting. We have started to study this reaction<br />
near the kinematical threshold. A proton beam of 1297 MeV/c from the<br />
Cosy accelerator has been used to test the experimental setup. For the<br />
detection of the recoiling nuclei, the magnetic spectrograph BIG KARL<br />
operates as a full solid angle detector. A new introduced detection system<br />
in the focal plane area being completely in vacuum ensures high<br />
kinematical resolution of the heavy recoil. Results of the test run as well<br />
as further detector improvements are discussed.<br />
HK 12.20 Tue 10:30 Foyer Chemie<br />
Deeply bound pionic states in Sn isotopes — •A. Gillitzer 1 , M.<br />
Fujita 2 , H. Geissel 3 , H. Gilg 4 , R.S. Hayano 5 , S. Hirenzaki 2 , K.<br />
Itahashi 6 , M. Iwasaki 6 , P. Kienle 4 , L. Maier 4 , M. Matos 3 , G.<br />
Münzenberg 3 , T. Ohtsubo 7 , M. Sato 6 , M. Shindo 5 , K. Suzuki 5 ,<br />
T. Suzuki 5 , H. Weick 3 , M. Winkler 3 , T. Yamazaki 8 , and T.<br />
Yoneyama 6 — 1 IKP, Forschungszentrum Jülich — 2 Nara Women’s<br />
University — 3 GSI Darmstadt — 4 Technische Universität München —<br />
5 University of Tokyo — 6 Tokyo Institute of Technology — 7 Niigata University<br />
— 8 RI Beam Science Lab., RIKEN<br />
The comparative measurement of binding energy and width of deeply<br />
bound pionic states in nuclei with different N/Z ratio allows to separately<br />
determine the isoscalar and the isovector part of the pion-nucleus potential.<br />
For this purpose the population of deeply bound pionic states in Sn<br />
isotopes was studied in a recent experiment at the GSI Fragmentseparator<br />
(FRS), using the (d, 3 He) reaction from <strong>11</strong>2,<strong>11</strong>6,120,124 Sn targets. The<br />
incident d beam kinetic energy was chosen to be 500 MeV in order to allow<br />
the formation of substitutional pionic 1s states coupled to 3s1/2 neutron<br />
hole states in recoilfree kinematics. Prominent peaks in the excitation<br />
energy spectrum corresponding to the pionic 1s state were observed in<br />
the irradiation of <strong>11</strong>6,120,124 Sn. First results of the data analysis will be<br />
presented.<br />
HK 12.21 Tue 10:30 Foyer Chemie<br />
Luminosity determination at COSY-<strong>11</strong> using the pd elastic scattering<br />
— •S .Steltenkampfor the COSY-<strong>11</strong> collaboration — Institut<br />
für Kernphysik, Universität Münster, Germany<br />
Measurements on the near-threshold η and η ′ meson production in<br />
the reaction channel pd → 3 HeX have been performed at the internal<br />
beam experiment COSY-<strong>11</strong> [1,2]. To extract total and differential cross<br />
sections, the proton-deuteron elastic scattering has been measured simultaneously<br />
as reference reaction for normalization purposes. Close to<br />
the η and η ′ meson production thresholds (pthr.,η = 1.570 GeV/c, pthr.,η ′<br />
= 2.434 GeV/c) the COSY-<strong>11</strong> facility allows for an identification and