Precession of the muon in a weak
and variable magnetic field can introduce
a time dependant modulation of the time distribution
of the measured muon decay, if there is any efficiency for
the detection system that varies with the electron decay angle.
The distortion depends on the muon spin polarization coefficent and
the decay asymmetry. We have observed this effect and we have
empirically corrected the time spectrum to minimize the
resulting
with an excellent fit.
To first order the cylindrical symmetry of our detector
eliminates this effect, however we wish to reduce it further
by actually measuring both the polarization and the residual detection
assymetries within our detector.
We will apply a uniform 70 Gauss field perpendicular to
the beam direction with the coils described previously. This
field precesses the remaining free muon polarization at 1 MHz
causing an easily fittable sinusoid on top of our decay spectrum.
Both the amount of polarization and the decay of that polarization
will be fit and removed from the decay curve. In the case
that there is a small transverse polarization or our coils
are not perfectly aligned we will also rotate the coil set by
90
to fully resolve the polarization vector and
correct for it. One other reason for rotating the field is to
spin the polarization past the other half of the detector so
we can measure the differential efficiencies of each opposing
element of our detector.
Little or no polarization should exist in the
experiment. However, we will look for polarization effects in
both
and
. The primary plan is to use the
magnetic field to allow us to check the
lifetime
reference with the same setup used for the
capture experiment.
Though the magnet is not necessary for the
capture
part we intend to leave the magnet in place for both runs
so that the experiments would have been done in identical
situations. In the outer position scattering in the magnet
materials will not significantly affect our traceback resolution.