Difference between revisions of "Elong-13-10-09b"
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− | ! colspan="2" | | + | ! colspan="2" | $E_{\mathrm{beam}}=6.6\mathrm{~GeV}$ |
|- | |- | ||
− | | | + | |$\mathrm{HMS~}\theta_{e'}=12.382^{\circ}$<br> |
− | + | $\mathrm{HMS~}E'=5.862\mathrm{~GeV}$<br> | |
− | + | $\mathrm{HMS~}Q^2=1.800\mathrm{~(GeV/}c)^2$<br> | |
− | || | + | ||$\mathrm{SHMS~}\theta_{e'}=8.231^{\circ}$<br> |
− | + | $\mathrm{SHMS~}E'=6.252\mathrm{~GeV}$<br> | |
− | + | $\mathrm{SHMS~}Q^2=0.850\mathrm{~(GeV/}c)^2$<br> | |
|- | |- | ||
| colspan="2" | '''1 Week Measurement'''<br> | | colspan="2" | '''1 Week Measurement'''<br> |
Latest revision as of 13:57, 18 October 2023
Azz Rates by Spectrometer
Same calculations as done for the combined optimized rates, except that they're now shown with the statistics that are contributed by each spectrometer. For this plot, the dilution factors were calculated individually for each spectrometer.
$E_{\mathrm{beam}}=6.6\mathrm{~GeV}$ | |
---|---|
$\mathrm{HMS~}\theta_{e'}=12.382^{\circ}$ $\mathrm{HMS~}E'=5.862\mathrm{~GeV}$ |
$\mathrm{SHMS~}\theta_{e'}=8.231^{\circ}$ $\mathrm{SHMS~}E'=6.252\mathrm{~GeV}$ |
1 Week Measurement | |
2 Week Measurement |
--E. Long 22:15, 8 October 2013 (UTC)