Difference between revisions of "Elong-13-10-09"
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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="5" | | + | ! colspan="5" | $E_{\mathrm{beam}}=11.0\mathrm{~GeV}$ |
|- | |- | ||
| − | | | + | |$\mathrm{HMS~}\theta_{e'}=12.523^{\circ}$<br> |
| − | + | $\mathrm{HMS~}E'=7.299\mathrm{~GeV}$<br> | |
| − | + | $\mathrm{HMS~}Q^2=3.820\mathrm{~(GeV/}c)^2$<br> | |
| − | || | + | ||$\mathrm{SHMS~1~}\theta_{e'}=7.346^{\circ}$<br> |
| − | + | $\mathrm{SHMS~1~}E'=6.701\mathrm{~GeV}$<br> | |
| − | + | $\mathrm{SHMS~1~}Q^2=1.210\mathrm{~(GeV/}c)^2$<br> | |
| − | || | + | ||$\mathrm{SHMS~2~}\theta_{e'}=8.962^{\circ}$<br> |
| − | + | $\mathrm{SHMS~2~}E'=7.447\mathrm{~GeV}$<br> | |
| − | + | $\mathrm{SHMS~2~}Q^2=2.000\mathrm{~(GeV/}c)^2$<br> | |
| − | || | + | ||$\mathrm{SHMS~3~}\theta_{e'}=9.848^{\circ}$<br> |
| − | + | $\mathrm{SHMS~3~}E'=7.958\mathrm{~GeV}$<br> | |
| − | + | $\mathrm{SHMS~3~}Q^2=2.580\mathrm{~(GeV/}c)^2$<br> | |
|- | |- | ||
| colspan="5" | '''30 Day Measurement'''<br> | | colspan="5" | '''30 Day Measurement'''<br> | ||
Latest revision as of 13:56, 18 October 2023
b1 With Updated Rates Code
Updated the b1 plots since I made a number of changes to the b1 rates code cross-sections. Using Pzz=30% and SHMS-3 setting for the dilution factor.
| $E_{\mathrm{beam}}=11.0\mathrm{~GeV}$ | ||||
|---|---|---|---|---|
| $\mathrm{HMS~}\theta_{e'}=12.523^{\circ}$ $\mathrm{HMS~}E'=7.299\mathrm{~GeV}$ |
$\mathrm{SHMS~1~}\theta_{e'}=7.346^{\circ}$ $\mathrm{SHMS~1~}E'=6.701\mathrm{~GeV}$ |
$\mathrm{SHMS~2~}\theta_{e'}=8.962^{\circ}$ $\mathrm{SHMS~2~}E'=7.447\mathrm{~GeV}$ |
$\mathrm{SHMS~3~}\theta_{e'}=9.848^{\circ}$ $\mathrm{SHMS~3~}E'=7.958\mathrm{~GeV}$ | |
| 30 Day Measurement
| ||||
--E. Long 22:16, 8 October 2013 (UTC)
