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The experiments with the polarized deuteron target and polarized He target
are listed in Table vii
with the year of their publish, average and integrated value of .
Motivation of both experiments to extract the spin-dependent structure function of
neutron.
Table vii: Polarized DIS experiments with polarized deuteron target and polarized He target.
In the case of He data, is listed instead of .
- CERN-SMC (93, 95) [16,21]
- The spin dependent structure function has been measured
using the 100 GeV and 190 GeV polarized muon beams at CERN. The beam polarization
has been determined from the energy spectrum of the positron from decay muon.
- The contribution from quadrupole structure function
is expected to be small and neglected.
- has been neglected. The depolarization has been evaluated
using in Ref. [15].
- SLAC-E143 [20]
- Similarly to the proton case, they have measured both and
using the polarized electrons of three energy points. All data
has been used to study dependence of the asymmetries. Only the data
with highest energy beam (29.1 GeV) was used to obtain the integral of
. We can use the data with other beam energies for our global
fit.
- The nuclear effect on asymmetry has been evaluated from the measured
polarization of nitrogen and shell model calculation to determine the contribution
of the unpaired p-shell proton.
- The depolarization has been evaluated
using in Ref. [15].
- E142 [17]
- The experiment utilized the polarized He target, which is the good
good model of polarized neutron target in DIS experiment.
The asymmetry has been corrected with the proton polarization
( per one proton), and neutron polarization ().
- The beam polarization has been measured with Moeller polarimeter as
38.81.6%.
- The He polarization has been measured with NMR technique as
30-40% 7%.
- The has been neglected since their measurements was
consistent with zero within a statistical accuracy (0.25).
Table viii: Experiments with deuteron.
Table ix: Kinematical coverage of each experiment and number of data
points are tabulated.
Table x: Corrections to the measured asymmetries. The effect of was neglected but
the uncertainty due to the effect has been estimated and included in the systematic uncertainty. In E142,
the measured asymmetry was consistent with zero within a statistical
error of 0.25, thus neglected in the analysis.
Next: Re-evaluation of Data
Up: Review of the Data
Previous: Proton Data
Saito Naohito
1996年10月13日 17時20分31秒