The electron beam is generated polarized by using circularly polarized laser light; the polarization is controlled by a Pockel cell.
In the initial implementation of the helicity scheme, there were two signals, hereafter called A and B , used to indicate the polarization state. For all labelling of cables, documentation, etc., the helicity scheme was defined to be:
| A | B | actual polarity |
|---|---|---|
| + | - | + |
| - | + | - |
These signals were generated at the source and coupled to the Hall A counting house, via optical fiber. For FPP test run, at the sub-ns level, one source signal would be logical true and the other would be logical false. The length of each helicity state was about 33 ms, the polarization in the Hall required about 100 microseconds to stabilize after the start of the change of the helicity, and + and - pulses alternated.
Important note: in replay in checking the phases, Ed Brash discovered that the phase convention listed above was backward. Hall C Moller confirmed. Accelerator stated that the phase convention was intended to be arbitrary, not A = + as we had believed.
For E89-033 running, it is planned to adopt a more uncorrelated scheme with a superperiod signal to allow parity parasite measurements. The convention is:
| A | B | superperiod | actual polarity |
|---|---|---|---|
| + | - | + | + |
| - | + | + | - |
| + | - | - | - |
| - | + | - | + |
At this point it is not clear that the scheme reflects the actual helicities from the source, or the reversed, misunderstood helicities, from before.
Some operational notes:
Created July 7, 1996 Ronald Gilman