Hadron structure is certainly not the sole province of the electromagnetic
community. Hadron structure studies are an active area of research in high
energy physics, particularly spectroscopic-type searches for states to fill
out the expected roster of the mesons and baryons. Results have been
obtained in experiments using probes such as radiative J/ decays and
antiproton annihilation at rest. Specifically electromagnetic results in
the area of hadron structure physics have been limited to the analyses of
older data in recent years due to the lack of suitable machines and beam
time. Effort has been concentrated on development of the programs of the
nucleon structure studies at CEBAF [Bu92], as well as a many planned
experiments using real or virtual photons to study strangeness production
and the spectroscopy of the meson sector [CE94] [St94].
New insights into nucleon structure was gained from the analysis of
inclusive electron scattering and of pion electroproduction data in the
resonance region [St91]. Unseparated transition form factors
for resonances in the and
mass regions indicate
scaling behavior at large momentum transfer, while such a behavior is not
observed for the
. The latter result is consistent with
results of pion production analysis, which shows the E2/M1 ratio to be
small even at
GeV
, while pQCD predicts this ratio to
approach unity. Leading order perturbative QCD contributions may therefore
still be relatively small for the
at these momentum transfers.
Analyses also showed that the helicity structure of the lower mass
resonance transitions, especially of the
, plays the dominant
role for explaining the underlying dynamics of the Drell-Hearn-Gerasimov
helicity sum rule and its connection with the deep inelastic spin sum
rules.
The E2/M1 mixing ratio in the N to transition (EMR) is a
particularly sensitive measure of spin-dependent quark-quark forces. In
constituent quark models, both the nucleon and the
are constructed
predominantly from orbital angular momentum
components. A quark-
quark tensor interaction, mediated by one-gluon exchange, introduces small
admixtures, which break spherical symmetry and results in ``deformed"
nucleons and
's. Predictions for the E2 transitions between these
states at
are quite small in constituent models, EMR = -(0.5 +/-
0.3)%, but significantly larger in models that explicitly contain pion
fields, eg. -(1.5 +/-0.5)%with Chiral bags or -(4.5 +/-1.5)%with
Skyrmions. (The negative phase of the EMR would correspond to an oblate
intrinsic shape.) The last five years have seen a record number of attempts
at extracting this small EMR value from old (mostly unpolarized) data.
The effects of E2 transitions can be enhanced through polarization
observables. A set of complete measurements of the
,
, and
reactions with polarized photons has recently been
completed at LEGS. The observed E2
are actually quite large, but
most of this results from interferences with E2 components of the Born
amplitudes, which are not particularly interesting. The E2 part associated
with the excitation of the
must be extracted by decomposing the
amplitudes into resonant + background components. Predictions including
only the background are several standard deviations per point away from the
new polarization data. Preliminary analyses of the new LEGS results, while
somewhat model dependent, are consistent with EMR =
% [Sa94].
Evidently, the
orbital angular momentum components in the N/
are much larger than expected in the constituent quark model.