The CB-ELSA Collaboration
Spokesperson: E. Klempt
Contact Person: J. Smyrski
e-mail: thoma@iskp.uni-bonn.de
J. Smyrski
Institute of Physics, University of Crakow
H. Flemming, H. Koch, H. Matthäy
Physikalisches Institut, Universität Bochum
O. Barholomy, V. Credé, A. Ehmanns, J. Ernst, I. Fabry, M. Fuchs, C.
Funke,
J. Junkersfeld, H. Kalinowsky, E. Klempt, C. Schmidt, T. Szczepanek, U. Thoma
Institut für Strahlen- und Kernphysik, Universität Bonn
Y.A. Beloglazov, A.B. Gridnev, I.V. Lopatin, D.V. Novinski, V.V. Sumachev
Leningrad Nuclear Physics Institute, Gatchina, St.Petersburg
and Institut für Strahlen- und Kernphysik, Universität Bonn
R. Bantes, H. Dutz, R. Gothe, E. Gutz, S. Höffgen, M.Konrad, B. Schoch,
D. Walther
and F. Klein, D. Menze, M. Ostrick
Physikalisches Institut, Universität Bonn
A. Kozela
Institute of Nuclear Physics, Crakow
G. Anton, A. Fösel, J. Hößl, G. Suft
Physikalisches Institut, Universität Erlangen
H. Freiesleben, B. Kopf, E. Kuhlmann
Physikalisches Institut, Universität Dresden
B. Krusche, V. Metag, R. Novotny, S. Sack, S. Schadmand
Physikalisches Institut, Universität Giessen
M. Schumacher, F. Smend, W. Weihofen
Physikalisches Institut, Universität Göttingen
J. Langheinrich, R. Santo
Physikalisches Institut, Universität Münster
Bonn, October 1999
Beam specifiations
e- beam | 3.2 / 1.5 / 1.0 GeV e- (un)-polarized |
beam line | SAPHIR beamline |
beam intensity | ~ 2 106 tagged photons/s |
time structure | continuous beam |
Equipment
The measurements will take place in the former SAPHIR area at ELSA using the
Crystal-Barrel detector and a scintillating fibre detector for tracking of charged
particles. The (upgraded) photon tagger of the SAPHIR experiment and a photon
veto counter behind the target define interactions of photons. The trigger requires
an interacting photon and energy deposit in the barrel detected in a fast cluster
encoder. The data will be taken in parallel to the accepted proposal on photoproduction
of .
Polarised electrons would be welcome but are not required.
Abstract
We propose to study the reaction with
the
and
both decaying into
.
Data on this reaction will allow
The Crystal Barrel detector with its excellent photon detection capability
is the ideal instrument to study this reaction over the full dynamical range.
We plan to perform the experiment in the SAPHIR area in which the Crystal Barrel
detector is presently being set up. The SAPHIR tagger will be used covering
a photon energy range from 0.31 to 0.94 times the primary electron energy.With
a choice of 3.2 GeV we cover from
1.67 to 2.55 GeV and thus reach an upper limit of 1.6 GeV in the
invariant
mass. At this energy, the predicted
production
cross section has its maximum value. In the set up phase we will use a second
setting in which we cover the photon energy range from 0.31 to 0.94 GeV. The
lower limit is at the nominal
production threshold, the energy range covers the second resonance region up
to
=1.62
GeV.
The 3rd resonance region will be investigated by the choice of an
e- beam momentum of 1.5 GeV providing a bridge between the two former
data sets. Interacting photons are defined by the tagger signal in anticoincidence
with the photon-veto, their energy is measured through the electron deflection
angle in the magnetic field of the tagger. We plan to trigger the data acquisition
by the presence of an interacting photon in coincidence with a multiplicity-one
signal from a scintillating fibre counter surrounding the 5 cm liquid H2
target and in coincidence with a fast photon-cluster encoder asking for at least
3 contiguous energy deposits in the Crystal Barrel.
We plan to start with a moderate beam intensity of ~ 2 106
tagged photons/s. The data will be taken simultaneously with data on other reactions;
in particular with data on production
(Proposal U. Thoma, 1998), on photoproduction of
and
'
mesons (Proposal A. Fösel, 1999) and of
and
(Proposal R. Gothe, 1999).