Privacy and Security Notice
procedure
Procedure for Hee'p checking 02/10/06
(rev. 02/13/06)
The procedure outlined below was performed for the Heep runs at Ebeam =
4.021 GeV and electron angle of 50.0 deg.
The Beam energy including energy loss in the target was determined by
printing out gpbeam in the Analyzer. The value was 4.02022
GeV.
The contributions from radiative corrections needed to be determined
first. SIMC was run at the same setting with the SOS out-of-plane
offset included. SIMC was run with and without radiative
corrections, and the results are shown below.
With Radiative corrections

|
Without radiative corrections

|
The difference (with rad - without rad) for each plot are:
W=
2.85883
Em= 0.47538
Pmpar= 0.79623
Pmper= -0.88237
Pmoop= 0.0963397
eCorsi= -1.13889
pCorsi= -0.42788
phi= -0.00416332
I will skip over the part where the offsets were determined by the
standard HallC code "heepcheck.f", and come back to this after the next
set of plots. So, for now, just assume we have determined some
offsets from the heep analysis. The offsets from the radiative
corrections were put into the kumac that calculated W, Em, Pmpar, etc,
and here are the results before the heep offsets were included and
after they were included. This shows that the heep offsets appear
reasonable and move the plots in the correct direction.
Before Hee'p offsets

|
After Hee'p offsets

|
The process of choosing the Hee'p offsets was rather subjective.
At first Eric Christy's automated program "autoheep.f" was used, and
the offsets used as input for this program were corrected for the beam
energy loss and radiative corrections (ie -7.33
MeV, -0.938 MeV, -6.91 MeV and 1.56 MeV from the LHS plot above).
Of the possible results, the ones with zero change in
beam energy were considered. Of the results left over, the
solution with the smallest chisq and with small changes in the
spectrometer angles was selected. Here is the complete output from the program.
The set of offsets selected was
dE=0.0
dth_ss=1.0
dp_ss=0.6
dth_hs=1.0
dp_hs=2.7
The plots using these optimized offsets are included below

I decided to try an alternative method for determining the optimized
offsets. Assuming the beam energy and spectrometer angles were
more accurate than the mometum, the momentum offsets for the electron
and proton were changed until the corrected singles plots (Corsi)
showed no offset. At this point, the offsets in the other plots
were
less than 2MeV, so, after this, only minor tweaking of the offsets was
performed.
Using the matrix in the heepcheck.f program as a guide, I adjusted the
beam energy, spectrometer angles and spectrometer momentum until all
the plots were close to being centered on zero. Here are the
offsets determined with this method:
dE=0.0
dth_ss=0.1
dp_ss=2.0
dth_hs=0.4
dp_hs=2.15
The plots using these optimized offsets are shown below. The
observed deviations from zero are smaller than those determined using
autoheep. Therefore, this method will be used for the other
settings.

Code used to generate this plot h.kumac
and myheepcheck.f.
Note- Just for interest. Here is the same plot without the RC
affects to show that I have the sign put in correctly for this
affect. The plots in the panel below all shift by a few MeV in
the direction of the tails compared to the previous panel.

See also a change to the procedure here
(02/16/06).
Another change to the procedure was also made here (03/28/06).