49 research outputs found
Isospin dependence of the eta prime meson production in nucleon-nucleon collisions
A comparison of the close-to-threshold total cross section for the eta prime
production in pp --> pp eta prime and pn --> pn eta prime reactions constitutes
a tool to investigate the eta prime meson structure and the reaction mechanism
in the channels of isospin I=0 and I=1 and may provide insight into the
flavour-singlet (perhaps also into gluonium) content of the eta prime meson. In
this contribution we present preliminary results of measurement of the
quasi-free production of the eta prime meson in the proton-neutron collisions
conducted using the COSY-11 facility.Comment: Presented at 10th International Workshop on Meson Production,
Properties and Interaction (MESON 2008), Cracow, Poland, 6 - 10 June 200
First close-to-threshold measurement of the analyzing power Ay in the reaction p(pol)p -> pp eta
At the internal facility COSY-11 a first measurement of the reaction p(pol)p
-> pp eta near the production threshold has been performed. Results for the
analysing power will be presented and a comparison with one meson exchange
models will be discussed.Comment: 3 pages, 3 figures, Presented at Conference on Quarks and Nuclear
Physics (QNP 2002), Julich, Germany, 9-14 Jun 200
New results on the pd --> 3He eta production near threshold
Measurements on the eta meson production in proton-deuteron collisions have
been performed using the COSY-11 facility at COSY Juelich. Here we present
preliminary results on total and differential cross sections for the pd --> 3He
eta reaction at five excess energies between Q = 5.1 and Q = 40.6 MeV. The
obtained angular distributions for the emitted eta mesons in the center of mass
system expose a transition from an almost isotropic emission to a highly
anisotropic distribution. The extracted total cross sections support a strong
eta-3He final state interaction and will be compared with model predictions.Comment: Presented at MESON 2004: 8th International Workshop on Meson
Production, Properties and Interactions, Cracow, Poland, 4-8 Jun 2004, 3
pages, Submitted to Int. J. Mod. Phys.
Total and Differential Cross Sections for the pp-->pp eta-prime Reaction Near Threshold
The eta-prime meson production in the reaction pp-->pp eta-prime has been
studied at excess energies of Q = 26.5, 32.5 and 46.6 MeV using the internal
beam facility COSY-11 at the cooler synchrotron COSY. The total cross sections
as well as one angular distribution for the highest Q-value are presented. The
excitation function of the near threshold data can be described by a pure
s-wave phase space distribution with the inclusion of the proton-proton final
state interaction and Coulomb effects. The obtained angular distribution of the
eta-prime mesons is also consistent with pure s-wave production.Comment: 6 pages, 5 figures, submitted to Eur. Phys. J.
Threshold Hyperon Production at COSY-11
The Lambda, Sigma0 and Sigma+ hyperon production in NN collisions is studied
at the COSY - 11 installation in order to investigate the production mechanism
as well as to extract information about the Y-N interaction.Comment: 3 pages, 2 figure
Search for Bremsstrahlung radiation in quasi-free n p --> n p gamma reactions
Due to the high sensitivity of the N N --> N N gamma reaction to the
nucleon-nucleon potential, Bremsstrahlung radiation is used as a tool to
investigate details of the nucleon-nucleon interaction. Such investigations can
be performed at the cooler synchrotron COSY in the Research Centre Juelich, by
dint of the COSY-11 detection system. The results of the identification of
Bremsstrahlung radiation emitted via the d p --> d p gamma reaction in data
taken with a proton target and a deuteron beam are presented and discussed.Comment: 3 pages; Presented at Meson 2004: 8th International Workshop on Meson
Production, Properties and Interaction, Krakow, Poland, 4-8 June 2004;
Submitted to International Journal of Modern Physics
Variation of nonequilibrium processes in p+Ni system with beam energy
The energy and angular dependence of double differential cross sections
dsigma/dOmega dE were measured for p, d, t, 3,4He, 6,7Li, 7,9Be, and 10,11B
produced in collisions of 0.175 GeV protons with Ni target. The analysis of
measured dfferential cross sections allowed to extract total production cross
sections for ejectiles listed above. The shape of the spectra and angular
distributions indicate the presence of other nonequilibrium processes besides
the emission of nucleons from the intranuclear cascade, and besides the
evaporation of various particles from remnants of intranuclear cascade. These
nonequilibrium processes consist of coalescence of nucleons into light charged
particles during the intranuclear cascade, of the fireball emission which
contributes to the cross sections of protons and deuterons, and of the break-up
of the target nucleus which leads to the emission of intermediate mass
fragments. All such processes were found earlier at beam energies 1.2, 1.9, and
2.5 GeV for Ni as well as for Au targets, however, significant differences in
properties of these processes at high and low beam energy are observed in the
present study.Comment: 10 pages, 9 figure
Competition of coalescence and "fireball" processes in nonequilibrium emission of light charged particles from p+Au collisions
The energy and angular dependence of double differential cross sections was
measured for p,d,t,He,Li,Be, and B isotopes produced in collisions of 1.2 and
1.9 GeV protons with Au target. The shape of the spectra and angular
distributions almost does not change in the beam energy range from 1.2 to 2.5
GeV, however, the absolute value of the cross sections increases for all
ejectiles. A phenomenological model of two emitting, moving sources reproduces
very well spectra and angular distributions of intermediate mass fragments.
Double differential cross sections for light charged particles (LCP) were
analyzed in the frame of the microscopic model of intranuclear cascade (INC)
with coalescence of nucleons and statistical model for evaporation of particles
from excited residual nuclei. Energy and angular dependencies of data agree
satisfactorily neither with predictions of microscopic intranuclear cascade
calculations for protons, nor with coalescence calculations for other LCP.
Phenomenological inclusion of another reaction mechanism - emission of LCP from
a "fireball", i.e., fast and hot moving source - combined with the microscopic
model calculations of INC, coalescence and evaporation of particles leads to
very good description of the data. It was found that nonequilibrium processes
are very important for production of LCP. They exhaust 40-80% of the total
cross sections - depending on the emitted particles. Coalescence and "fireball"
emission give comparable contributions to the cross sections with exception of
3He data where coalescence clearly dominates. The ratio of sum of all
nonequilibrium processes to those proceeding through stage of statistical
equilibrium does almost not change in the beam energy range from 1.2 GeV to 2.5
GeV for all light charged particles.Comment: 14 pages, 12 figures, IV tables, \pacs{25.40.-h,25.40.Sc,25.40.Ve
Asymptotic normalization coefficients from the (20)Ne((3)He, d)(21)Na reaction and astrophysical factor for (20)Ne(p,gamma)(21)Na
Journals published by the American Physical Society can be found at http://publish.aps.org/The (20)Ne(p,gamma)(21)Na reaction rate at stellar energies is dominated by capture to the ground state through the tail of a subthreshold resonance state at an excitation energy of 2425 keV in (21)Na. Both resonant and direct capture contribute to the reaction rate while direct captures to other bound states are negligible. The overall normalization of direct capture to the subthreshold state is determined by the asymptotic normalization coefficient (ANC). Simultaneously this ANC determines the proton partial width of the subthreshold resonance state. To determine the ANC, the (20)Ne((3)He,d)(21)Na proton transfer reaction has been measured, at an incident energy of 25.83 MeV. Angular distributions for proton transfer to the ground and first three excited states were measured, and ANCs were then extracted from comparison with distorted-wave Born approximation calculations. Using these ANCs, we calculated the astrophysical factor for (20)Ne(p,gamma)(21)Na. Our total astrophysical factor is S(0)=5900 +/- 1200 keV b. Our analysis confirms that only nonresonant and resonant captures through the subthreshold state are important
Near threshold production of the eta meson via the quasi-free pn --> pn eta reaction
Total cross sections for the quasi-free pn --> pn eta reaction in the range
from the kinematical threshold up to 20 MeV excess energy have been determined.
At threshold they exceed corresponding cross sections for the pp --> pp eta
reaction by a factor of about three in contrast to the factor of six
established for higher excess energies. To large extent, the observed decrease
of the ratio sigma(pn --> pn eta)/sigma(pp --> pp eta) towards threshold may be
assigned to the different energy dependence of the proton-proton and
proton-neutron final state interactions.
The experiment has been conducted using a proton beam of the cooler
synchrotron COSY and a cluster jet deuteron target. The proton-neutron
reactions were tagged by the spectator proton whose momentum was measured for
each event. Protons and neutron outgoing from the pn --> pn eta reaction have
been registered by means of the COSY-11 facility, an apparatus dedicated for
threshold meson production.Comment: 15 pages, 6 figures, submitted to Phys. Rev.