Difference between revisions of "Elong-13-10-09c"
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{| class="wikitable" style="text-align:center; border-collapse:collapse;" border="1" | {| class="wikitable" style="text-align:center; border-collapse:collapse;" border="1" | ||
| − | ! colspan="2" | <math>E_{\mathrm{beam}}= | + | ! colspan="2" | <math>E_{\mathrm{beam}}=6.6\mathrm{~GeV}</math> |
|- | |- | ||
|<math>\mathrm{HMS~}\theta_{e'}=10.766^{\circ}</math><br> | |<math>\mathrm{HMS~}\theta_{e'}=10.766^{\circ}</math><br> | ||
| Line 38: | Line 38: | ||
| colspan="2" | [[Image:2013-10-09c-e-66-opt.png]] | | colspan="2" | [[Image:2013-10-09c-e-66-opt.png]] | ||
|- | |- | ||
| + | | colspan="2" | '''Note: This is a best case scenario, where the minimum HMS angle is allowed to drop to <math>10.5^{\circ}</math>, instead of the <math>12.2^{\circ}</math> I've previously been using.''' | ||
|} | |} | ||
Revision as of 15:18, 9 October 2013
Azz with Matching Q^2
At with beam energies of 4.4 and 6.6 GeV, I attempted to optimize the rates while keeping both spectrometers at the same Q^2 which was above 1. I also added a cut so that only Q2>1 events are considered "good."
4.4 GeV Results
| <math>E_{\mathrm{beam}}=4.4\mathrm{~GeV}</math> | |
|---|---|
| <math>\mathrm{HMS~}\theta_{e'}=15.180^{\circ}</math> <math>\mathrm{HMS~}E'=3.908\mathrm{~GeV}</math> |
<math>\mathrm{SHMS~}\theta_{e'}=15.180^{\circ}</math> <math>\mathrm{SHMS~}E'=3.908\mathrm{~GeV}</math> |
| |
6.6 GeV Results
| <math>E_{\mathrm{beam}}=6.6\mathrm{~GeV}</math> | |
|---|---|
| <math>\mathrm{HMS~}\theta_{e'}=10.766^{\circ}</math> <math>\mathrm{HMS~}E'=6.026\mathrm{~GeV}</math> |
<math>\mathrm{SHMS~}\theta_{e'}=9.898^{\circ}</math> <math>\mathrm{SHMS~}E'=6.108\mathrm{~GeV}</math> |
| |
| Note: This is a best case scenario, where the minimum HMS angle is allowed to drop to <math>10.5^{\circ}</math>, instead of the <math>12.2^{\circ}</math> I've previously been using. | |
