There are a number of differences between the capabilities of the HAPPEX and
G0
experiments. Most importantly, because of the relatively small acceptance of
the Hall A spectrometers, the HAPPEX measurement is restricted to forward angle
asymmetries. Therefore, no direct extraction of
and
is possible
in the HAPPEX experiment. Secondly, for the forward angle asymmetries, the
statistical precision is limited by the acceptances of the spectrometers. In
the case of G0, forward angle asymmetries will be measured at seven values of
momentum transfer concurrently as shown in
Figure 6. The
statistical precision shown here is that for the experiment as proposed in 1993
with 49% beam polarization and a 30 day run. For comparison, the published
result from the recent HAPPEX run is also shown. The HAPPEX plans for 1999 are
to reduce the uncertainties by a factor of two with increased running time and
improved polarization. HAPPEX also proposed 4 other forward angle asymmetries
at momentum transfers ranging from 0.268 to 1.295 GeV2. The momentum
transfer of the present measurement is slightly below the maximum in the
figure-of-merit which drops off by a
% for each of the extreme
values of momentum transfer above.
Even though there is overlap in the approved kinematic ranges of the two experiments, there are clearly significant differences in the instrumentation and techniques for the two measurements. The two measurements are therefore complementary and will provide an important mutual cross check of results.
Jefferson Lab has approved parity-violation measurements with both
2H and 4He targets. The 2H measurement proposed in E91-010 is for
forward angles and is focussed on strange quark effects. The 2H measurement
proposed for the G0 experiment is a single backward angle measurement at
GeV2 used to determine the contribution of the axial radiative
correction to the asymmetries (this will complement the measurement of a similar
quantity at low momentum transfer in the deuterium part of the SAMPLE experiment
at Bates).
The approved experiments for 4He are at low momentum transfer (
GeV2 : 91-010) and moderate momentum transfer (
GeV2 : 91-004).
These experiments will determine
in the
4He nucleus and are therefore
complementary to direct measurements on the proton.
There has been some discussion of the sensitivity of, in particular, polarized
photoproduction [He92, Ti97, Ti98] to test hypotheses of knocking out
pairs from
the nucleon (E93-022). Such measurements again provide
complementary information as the nucleon matrix elements probed are more
complicated overlaps. These also depend to a significant degree on models for
their extraction.