499 research outputs found
Role of the baryon resonances in the eta and K+ photoproduction processes on the proton
Very recent eta and K+ photoproduction data on the proton from threshold up
to E = 2.6 GeV are interpreted within a chiral constituent quark formalism,
which embodies all known nucleon and hyperon resonances. Possible contributions
from an additional S11 resonance are presented.Comment: 12 pages, Part of NSTAR 2004 proceeding
Mesons electromagnetic production study via a constituent quark approach
Using a chiral constituent quark approach based on the broken SU(6) \otimes
O(3) symmetry, we focus on the spectroscopy of isospin-1/2 nucleonic
resonances. A model for the eta photoproduction, embodying all known nucleonic
resonances, shows clear need for a yet undiscovered S11 resonance, for which we
determine the mass (1.730 GeV) and the total width (180 MeV).Comment: 6 pages, Invited talk given at "International Workshop on Physics
with GeV Electrons and Gamma-Rays", Sendai, February 13 -15, 200
Quark Model Study of The eta Photoproduction: Evidence for a New S11 Resonance?
An extensive and systematic study of the recent eta photoproduction data up
to 1.2 GeV is presented within a chiral constituent quark model. A model
embodying all known nucleonic resonances shows clear need for a yet
undiscovered third S11 resonance in the second resonance region, for which we
determine the mass (1.729 GeV) and the total width (183 MeV). Furthermore, we
extract the configuration mixing angles, an important property of the
quark-quark interaction in the quark model, for the resonances S11(1535) and
S11(1650), as well as for the resonances D13(1520) and D13(1700). Our results
agree well with the quark model predictions. In addition, the partial eta N
decay widths and/or the photo-excitation helicity amplitudes for the nucleonic
resonances S11(1535), S11(1650), P11(1710), P13(1720), D13(1520), D13(1700),
D15(1675), and F15(1680) are also obtained in this approach.Comment: 25 pages, 5 figures, submitted to Eur. Phys.
Strangeness magnetic form factor of the proton in the extended chiral quark model
Background: Unravelling the role played by nonvalence flavors in baryons is
crucial in deepening our comprehension of QCD. Strange quark, a component of
the higher Fock states in baryons, is an appropriate tool to investigate
nonperturbative mechanisms generated by the pure sea quark.
Purpose: Study the magnitude and the sign of the strangeness magnetic moment
and the magnetic form factor () of the proton.
Methods: Within an extended chiral constituent quark model, we investigate
contributions from all possible five-quark components to and in the four-vector momentum range (GeV/c). Probability
of the strangeness component in the proton wave function is calculated
employing the model.
Results: Predictions are obtained without any adjustable parameters.
Observables and are found to be small and negative,
consistent with the lattice-QCD findings as well as with the latest data
released by the PVA4 and HAPPEX Collaborations.
Conclusions: Due to sizeable cancelations among different configurations
contributing to the strangeness magnetic moment of the proton, it is
indispensable to (i) take into account all relevant five-quark components and
include both diagonal and non-diagonal terms, (ii) handle with care the
oscillator harmonic parameter and the component
probability.Comment: References added, typos corrected, accepted for publication by Phys.
Rev.
Dynamical coupled-channel approach to hadronic and electromagnetic production of kaon-hyperon on the proton
A dynamical coupled-channel formalism for processes and
is presented which provides a comprehensive investigation of
recent data on the reaction. The non-resonant
interactions within the subspace are derived from effective
Lagrangians, using a unitary transformation method. The calculations of
photoproduction amplitudes are simplified by casting the coupled-channel
equations into a form such that the empirical amplitudes
are input and only the parameters associated with the channel are
determined by performing -fits to all of the available data for and . Good
agreement between our models and those data are obtained. In the fits to channels, most of the parameters are constrained within of
the values given by the Particle Data Group and/or quark model predictions,
while for parameters, ranges compatible with broken
symmetry are imposed. The main reaction mechanisms in photoproduction are singled out and issues related to newly suggested
resonances , , and are studied. Results illustrating
the importance of using a coupled-channel treatment are reported. Meson cloud
effects on the transitions are also discussed.Comment: Accepted Physical Review
Intrinsic charm content of the nucleon and charmness-nucleon sigma term
In the extended chiral constituent quark model, the intrinsic
content of the nucleon is investigated. The probabilities of the
quark-antiquark components in the nucleon wave functions are calculated by
taking the nucleon to be admixtures of three- and five-quark components, with
the relevant transitions handled {\it via} the P mechanism.
Predictions for the probability of the in the nucleon wave function
and the charmness-nucleon sigma term are presented. Our numerical results turn
out to be consistent with the predictions from various other approaches
reported in the literature.Comment: Accepted for publication in Phys. Rev.
Dynamical coupled-channel model of kaon-hyperon interactions
The pi N --> KY and KY --> KY reactions are studied using a dynamical
coupled-channel model of meson-baryon interactions at energies where the baryon
resonances are strongly excited. The channels included are: pi N, K \Lambda,
and K\Sigma. The resonances considered are: N^* [S_{11}(1650), P_{11}(1710),
P_{13}(1720),D_{13}(1700)]; \Delta^* [S_{31}(1900), P_{31}(1910),
P_{33}(1920)]; \Lambda ^* [S_{01}(1670), P_{01}(1810)] \Sigma^* [P_{11}(1660),
D_{13}(1670)]; and K^*(892). The basic non-resonant \pi N --> KY and KY --> KY
transition potentials are derived from effective Lagrangians using a unitary
transformation method. The dynamical coupled-channel equations are simplified
by parametrizing the pi N -->pi N amplitudes in terms of empirical pi N
partial-wave amplitudes and a phenomenological off-shell function. Two models
have been constructed. Model A is built by fixing all coupling constants and
resonance parameters using SU(3) symmetry, the Particle Data Group values, and
results from a constituent quark model. Model B is obtained by allowing most of
the parameters to vary around the values of model A in fitting the data. Good
fits to the available data for pi^- p to K^0 \Lambda, K^0 \Sigma^0 have been
achieved. The investigated kinematics region in the center-of-mass frame goes
from threshold to 2.5 GeV. The constructed models can be imbedded into
associated dynamical coupled-channel studies of kaon photo- and
electro-production reactions.Comment: 35 pages, 11 Figure
Coupled channel study of photoproduction
A coupled channel model with , and channels has been
used to analyze the recent data of . The non-resonant
interactions within the subspace are derived from effective
Lagrangians using a unitary transformation method. The direct photoproduction
reaction is obtained from a chiral constituent quark model with breaking. Missing baryon resonances issues are briefly discussed.Comment: Part of the proceedings of the International Workshop on the Physics
of Excited Baryons NSTAR05, 12-15 October 2005, Tallahassee, Florida, US
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