Analysis Meeting 1
1) All 3 BCM Calibration runs were analyzed and fit linearly
for BCM1,2 Freq. vs. Unser Current (I). Between all the runs
there was a very small difference in the offset and gain measured.
2) We've begun to analyze the Efficiencies for the Calorimeter,
Cerenkov, and Tracking yet we are in the midst of replaying
the newly calibrated data so results are decent but not fantastic.
3) I've inspected the kinematics for each run by comparing the
data on the run sheet to the JPEG files for the HMS and SOS angles.
I've found a small amount of human error in what was recorded (~2% of
all runs).



Efficiencies - Preliminary
Note: We are expecting to redo these with the newly calibrated data.
These results are not to be taken seriously.
Calorimeter Efficiency
To identify only electrons and not pions are being measured, we apply the following cuts:
Ecalo/E' >0.7
Cer> 8
where Ecalo/E' is the energy recieved in the calorimeter divided by the energy
of the outgoing particle. For electrons, we expect them to deposit all their
energy in the Calo. such that Ecalo/E' ~ 1.
Cer denotes the # of photoelectrons produced in the Cerenkov
detector. For pions, we know the # of p.e. is about zero and for
electrons ~10 p.e. are produced.
Our formula for efficiency is then:
Eff(Calo) = Events (Ecalo/E' > 0.7 & Cer >8) / Events (Cer > 8)
The three points that are off the curve for low E' might be that way due to lack of
calibration or loss of efficiency at that momentum.

Cerenkov Efficiency
The cuts applied here were:
Ecalo/E' > 1.05
Cer > 2
Ecalo/E' has been raised to restrict any contamination by pions where Cer has
been lowered to hopfully include all electrons detected.
Efficiency is then:
Eff(Cer) = Events ( Cer >2 & Ecalo/E' > 1.05) / Events (Ecalo/E'>1.05)
Again we find low efficiciency at low E' which is likely due to uncalibration.
Tracking Efficiency
Eff(Tracking) = (TRG & PID & TR) / (TRG & PID)
where TRG: formed trigger, TR: found track, PID: particle id cut


