70 research outputs found
Recent Advances in Dyson-Schwinger Studies
There have been many demonstrations of the utility of the Dyson-Schwinger
equations of QCD as a systematic, phenomenological framework for describing the
perturbative and non-perturbative dynamics of hadrons in terms of Euclidean
Green functions of quarks and gluons. Still, there remain some unanswered
questions regarding the theoretical underpinnings of the approach. I review
several studies that are shedding light on how these questions might be
resolved and review predictions for some exotic meson states.Comment: Plenary talk at N-Star 2002. 5 pages, 3 figure
Current Conservation in the Covariant Quark-Diquark Model of the Nucleon
The description of baryons as fully relativistic bound states of quark and
glue reduces to an effective Bethe-Salpeter equation with quark-exchange
interaction when irreducible 3-quark interactions are neglected and separable
2-quark (diquark) correlations are assumed. This covariant quark-diquark model
of baryons is studied with the inclusion of the quark substructure of the
diquark correlations. In order to maintain electromagnetic current conservation
it is then necessary to go beyond the impulse approximation. A conserved
current is obtained by including the coupling of the photon to the exchanged
quark and direct ``seagull'' couplings to the diquark structure. Adopting a
simple dynamical model of constituent quarks and exploring various
parametrisations of scalar diquark correlations, the nucleon Bethe-Salpeter
equation is solved and the proton and neutron electromagnetic form factors are
calculated numerically. The resulting magnetic moments are still about 50% too
small, the improvements necessary to remedy this are discussed. The results
obtained in this framework provide an excellent description of the electric
form factors (and charge radii) of the proton, up to a photon momentum transfer
of 3.5GeV^2, and the neutron.Comment: 30 Pages, LaTeX2e, revised version, minor modifiactions to the text,
some phrases eliminated, some remarks adde
Non-diffractive mechanisms in the meson photoproduction on nucleons
We examine the non-diffractive mechanisms in the meson photoproduction
from threshold up to a few GeV using an effective Lagrangian in a constituent
quark model. The new data from CLAS at large angles can be consistently
accounted for in terms of {\it s}- and {\it u}-channel processes. Isotopic
effects arising from the reactions and , are investigated by comparing the cross sections and polarized beam
asymmetries. Our result highlights an experimental means of studying
non-diffractive mechanisms in meson photoproduction.Comment: 4 eps figures, version accepted by Phys. Lett.
Electromagnetic form factors of light vector mesons
The electromagnetic form factors G_E(q^2), G_M(q^2), and G_Q(q^2), charge
radii, magnetic and quadrupole moments, and decay widths of the light vector
mesons rho^+, K^{*+} and K^{*0} are calculated in a Lorentz-covariant,
Dyson-Schwinger equation based model using algebraic quark propagators that
incorporate confinement, asymptotic freedom, and dynamical chiral symmetry
breaking, and vector meson Bethe-Salpeter amplitudes closely related to the
pseudoscalar amplitudes obtained from phenomenological studies of pi and K
mesons. Calculated static properties of vector mesons include the charge radii
and magnetic moments: r_{rho+} = 0.61 fm, r_{K*+} = 0.54 fm, and r^2_{K*0} =
-0.048 fm^2; mu_{rho+} = 2.69, mu_{K*+} = 2.37, and mu_{K*0} = -0.40. The
calculated static limits of the rho-meson form factors are similar to those
obtained from light-front quantum mechanical calculations, but begin to differ
above q^2 = 1 GeV^2 due to the dynamical evolution of the quark propagators in
our approach.Comment: 8 pages of RevTeX, 5 eps figure
Spin Information from Vector-Meson Decay in Photoproduction
For the photoproduction of vector mesons, all single and double spin
observables involving vector meson two-body decays are defined consistently in
the center of mass. These definitions yield a procedure for
extracting physically meaningful single and double spin observables that are
subject to known rules concerning their angle and energy evolution. As part of
this analysis, we show that measuring the two-meson decay of a photoproduced
or does not determine the vector meson's vector polarization, but
only its tensor polarization. The vector meson decay into lepton pairs is also
insensitive to the vector meson's vector polarization, unless one measures the
spin of one of the leptons. Similar results are found for all double spin
observables which involve observation of vector meson decay. To access the
vector meson's vector polarization, one therefore needs to either measure the
spin of the decay leptons, make an analysis of the background interference
effects or relate the vector meson's vector polarization to other accessible
spin observables.Comment: 22 pages, 3 figure
Nucleonic resonance excitations with linearly polarized photon in
In this work, an improved quark model approach to the meson
photo-production with an effective Lagrangian is presented. The {\it t}-channel
{\it natural}-parity exchange is taken into account through the Pomeron
exchange, while the {\it unnatural}-parity exchange is described by the
exchange. With a very limited number of parameters, the available experimental
data in the low energy regime can be consistently accounted for. We find that
the beam polarization observables show sensitivities to some {\it s}-channel
individual resonances in the quark model symmetry limit.
Especially, the two resonances and , which belong
to the representation , have dominant contributions
over other excited states. Concerning the essential motivation of searching for
"missing resonances" in meson photo-production, this approach provides a
feasible framework, on which systematic investigations can be done.Comment: 16 pages, Revtex, 9 eps figures, to appear in PR
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