A sample plot of channeltron currents
, against electron gun
beam current
, for each of the opposite magnetization directions
used is given in figure 3.5, with the best fit lines whose
gradients were used to represent the electron arrival rates
(equation 2.4.) The change, on magnetization reversal, in the
difference between the gradients for the two channeltrons, which
represents the reflected beam polarization, is clearly visible.
![]() |
Similar data were also taken for two other beam energies, and the whole experiment was run twice to verify its repeatability.