From: Glen Warren (gwarren_at_anti-spam)
Date: 05-Jun-2003 09:56:44
GEn01 analysis meeting June 4, 2003 ==================================== attended by: Donal, Paul, Oscar at UVa Hongguo, Frank, Nikolai and Glen at JLab REPORTS *) GMn: We agreed to take the average of the Kelly and Basel Gmn and use the difference as the uncertainty. Thus, Gmn is: Q2=0.5: 1.013 +- 0.011 Q2=1.0: 1.063 +- 0.018 The approach for the paper will be that we extract Gen assuming Gmn=Dipole. We will give the number. Next, we will state that we know Gmn is not dipole, comment that the correction is mostly linear, and then give an extracted value of Gen. Mostly, it comes down to wording. *) Background: not results *) packing fraction for stick 4: Glen was concerned that the packing fraction for stick 4 doesn't have the proper weighting because the two cells have different packing fractions. Nikolai said that the p.f. are event weighted using all of the runs, so the reported p.f. do the proper averaging. *) dilution factor for stick 3: Hongguo's needs info on Kel-F. *) hszbeam cut for Q2=0.5: Glen repeat the hszbeam cut to examine the 4K shield contributions for Q2=0.5. The fit was not stable because of the smaller tails due to the smaller 4K shield contribution. His results are consistent with Nikolai's earlier findings, although just barely. The difficulty performing the fit makes the uncertainties in this approach large. Conclusion was that we get a smaller uncertainty for Q2=0.5 using the previous approach (no hszbeam cut, treat 4K shield as known dilution, don't include in d.f. model). *) CEX: Marko said that the size of the uncertainties for Q2=1.0 are much greater than the bin-by-bin dependence, so it is not worth doing a bin-by-bin correction. We reviewed the CEX bin-by-bin corrections for Q2=0.5 and reached the same conclusion. *) paper: Donal gave Glen a copy. Now there will be two people who don't have much time to work on it. *) variables to fit: Glen will write down his opinion to give us a starting point for discussion. Frank also wanted a justification for binning. *) kinematic uncertainties: We had a long discussion of exactly what to do. In the end we reached no conclusions. Glen will discuss matters with Frank to come up with something agreeable. *) Q2=0.5 fourth pass: Frank is calling it Fourth pass to be parallel to Q2=1, even though we do not have a Q2=0.5 third pass. It is about 1/3 done. Frank also noted that it was necessary to modify batchman to work with the new changes on the farm. *) Target polarization: Paul has submitted a new file with target polarization. The biggest difference is the better calculation of the length of the run. He uses the clock time for the start and the number of helicity buckets to get the length of the run. He also included correct B field, LHe level. There are 5 runs in which we He dropped below the cell and we continued to take data. These runs should be excluded from analysis. Paul present a plot showing the differences in the old and new target polarizations. The biggest differences in polarization occur mostly when the is a very large change in the length of the run. One curiosity appeared in that there were a lot of runs that previously had been 1-3 minutes long that were now ~73 m long. Glen thinks that the strong spike at 73 minutes is quite odd, suggestive of an error. There is also a broader hump around 35 minutes. *) pion production contributions: 0.44% for Q2=1. Done by adjusting the pion production to fit the data without cuts and then look at what survives the cuts. The issue of how to correct for this arose. We need to measure the asymmetry, which can be estimated by looking at the asymmetry for higher W. We need to remove the E' and theta_nq cut to see these pion events. *) Dilution Factor uncertainties: Nikolai will give Hongguo rates are varies target materials for Q2=1 for Hongguo to look at d.f. uncertainties. TO DO Donal *) work on paper. Glen *) look at 98 and 01 field setting codes *) work on paper *) write down approach of which variables to use for fit. *) Discuss with Frank the approach to kinematic uncertainties. Nikolai *) Give Hongguo rates are various target materials for Q2=1 Frank *) accidentals *) pion production asymmetries Hongguo *) dilution factor for stick 3 using path lengths thru materials. *) kinematic uncertainties *) dilution factor uncertainties
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