Difference between revisions of "Elong-13-10-09c"
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| − | ==Azz with | + | ==Azz with Q^2>1== |
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." | 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." | ||
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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" | | + | ! colspan="2" | $E_{\mathrm{beam}}=4.4\mathrm{~GeV}$ |
|- | |- | ||
| − | | | + | |$\mathrm{HMS~}\theta_{e'}=15.180^{\circ}$<br> |
| − | + | $\mathrm{HMS~}E'=3.908\mathrm{~GeV}$<br> | |
| − | + | $\mathrm{HMS~}Q^2=1.200\mathrm{~(GeV/}c)^2$<br> | |
| − | || | + | ||$\mathrm{SHMS~}\theta_{e'}=15.180^{\circ}$<br> |
| − | + | $\mathrm{SHMS~}E'=3.908\mathrm{~GeV}$<br> | |
| − | + | $\mathrm{SHMS~}Q^2=1.200\mathrm{~(GeV/}c)^2$<br> | |
|- | |- | ||
| colspan="2" | [[Image:2013-10-09c-e-44-opt.png]] | | colspan="2" | [[Image:2013-10-09c-e-44-opt.png]] | ||
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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" | | + | ! colspan="2" | $E_{\mathrm{beam}}=6.6\mathrm{~GeV}$ |
|- | |- | ||
| − | | | + | |$\mathrm{HMS~}\theta_{e'}=10.766^{\circ}$<br> |
| − | + | $\mathrm{HMS~}E'=6.026\mathrm{~GeV}$<br> | |
| − | + | $\mathrm{HMS~}Q^2=1.400\mathrm{~(GeV/}c)^2$<br> | |
| − | || | + | ||$\mathrm{SHMS~}\theta_{e'}=9.898^{\circ}$<br> |
| − | + | $\mathrm{SHMS~}E'=6.108\mathrm{~GeV}$<br> | |
| − | + | $\mathrm{SHMS~}Q^2=1.200\mathrm{~(GeV/}c)^2$<br> | |
|- | |- | ||
| 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 $10.5^{\circ}$, instead of the $12.2^{\circ}$ I've previously been using.''' | ||
|} | |} | ||
| + | |||
| + | |||
| + | --[[User:Ellie|E. Long]] 20:18, 9 October 2013 (UTC) | ||
Latest revision as of 13:57, 18 October 2023
Azz with Q^2>1
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
| $E_{\mathrm{beam}}=4.4\mathrm{~GeV}$ | |
|---|---|
| $\mathrm{HMS~}\theta_{e'}=15.180^{\circ}$ $\mathrm{HMS~}E'=3.908\mathrm{~GeV}$ |
$\mathrm{SHMS~}\theta_{e'}=15.180^{\circ}$ $\mathrm{SHMS~}E'=3.908\mathrm{~GeV}$ |
| |
6.6 GeV Results
| $E_{\mathrm{beam}}=6.6\mathrm{~GeV}$ | |
|---|---|
| $\mathrm{HMS~}\theta_{e'}=10.766^{\circ}$ $\mathrm{HMS~}E'=6.026\mathrm{~GeV}$ |
$\mathrm{SHMS~}\theta_{e'}=9.898^{\circ}$ $\mathrm{SHMS~}E'=6.108\mathrm{~GeV}$ |
| |
| Note: This is a best case scenario, where the minimum HMS angle is allowed to drop to $10.5^{\circ}$, instead of the $12.2^{\circ}$ I've previously been using. | |
--E. Long 20:18, 9 October 2013 (UTC)
