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}}=4.4\mathrm{~GeV}</math>
+
! colspan="2" | $E_{\mathrm{beam}}=4.4\mathrm{~GeV}$
 
|-
 
|-
−
|<math>\mathrm{HMS~}\theta_{e'}=15.180^{\circ}</math><br>
+
|$\mathrm{HMS~}\theta_{e'}=15.180^{\circ}$<br>
−
<math>\mathrm{HMS~}E'=3.908\mathrm{~GeV}</math><br>
+
$\mathrm{HMS~}E'=3.908\mathrm{~GeV}$<br>
−
<math>\mathrm{HMS~}Q^2=1.200\mathrm{~(GeV/}c)^2</math><br>
+
$\mathrm{HMS~}Q^2=1.200\mathrm{~(GeV/}c)^2$<br>
−
||<math>\mathrm{SHMS~}\theta_{e'}=15.180^{\circ}</math><br>
+
||$\mathrm{SHMS~}\theta_{e'}=15.180^{\circ}$<br>
−
<math>\mathrm{SHMS~}E'=3.908\mathrm{~GeV}</math><br>
+
$\mathrm{SHMS~}E'=3.908\mathrm{~GeV}$<br>
−
<math>\mathrm{SHMS~}Q^2=1.200\mathrm{~(GeV/}c)^2</math><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" | <math>E_{\mathrm{beam}}=6.6\mathrm{~GeV}</math>
+
! colspan="2" | $E_{\mathrm{beam}}=6.6\mathrm{~GeV}$
 
|-
 
|-
−
|<math>\mathrm{HMS~}\theta_{e'}=10.766^{\circ}</math><br>
+
|$\mathrm{HMS~}\theta_{e'}=10.766^{\circ}$<br>
−
<math>\mathrm{HMS~}E'=6.026\mathrm{~GeV}</math><br>
+
$\mathrm{HMS~}E'=6.026\mathrm{~GeV}$<br>
−
<math>\mathrm{HMS~}Q^2=1.400\mathrm{~(GeV/}c)^2</math><br>
+
$\mathrm{HMS~}Q^2=1.400\mathrm{~(GeV/}c)^2$<br>
−
||<math>\mathrm{SHMS~}\theta_{e'}=9.898^{\circ}</math><br>
+
||$\mathrm{SHMS~}\theta_{e'}=9.898^{\circ}$<br>
−
<math>\mathrm{SHMS~}E'=6.108\mathrm{~GeV}</math><br>
+
$\mathrm{SHMS~}E'=6.108\mathrm{~GeV}$<br>
−
<math>\mathrm{SHMS~}Q^2=1.200\mathrm{~(GeV/}c)^2</math><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 <math>10.5^{\circ}</math>, instead of the <math>12.2^{\circ}</math> I've previously been using.'''
+
| 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

$E_{\mathrm{beam}}=4.4\mathrm{~GeV}$
$\mathrm{HMS~}\theta_{e'}=15.180^{\circ}$

$\mathrm{HMS~}E'=3.908\mathrm{~GeV}$
$\mathrm{HMS~}Q^2=1.200\mathrm{~(GeV/}c)^2$

 $\mathrm{SHMS~}\theta_{e'}=15.180^{\circ}$

$\mathrm{SHMS~}E'=3.908\mathrm{~GeV}$
$\mathrm{SHMS~}Q^2=1.200\mathrm{~(GeV/}c)^2$

2013-10-09c-e-44-opt.png

6.6 GeV Results

$E_{\mathrm{beam}}=6.6\mathrm{~GeV}$
$\mathrm{HMS~}\theta_{e'}=10.766^{\circ}$

$\mathrm{HMS~}E'=6.026\mathrm{~GeV}$
$\mathrm{HMS~}Q^2=1.400\mathrm{~(GeV/}c)^2$

 $\mathrm{SHMS~}\theta_{e'}=9.898^{\circ}$

$\mathrm{SHMS~}E'=6.108\mathrm{~GeV}$
$\mathrm{SHMS~}Q^2=1.200\mathrm{~(GeV/}c)^2$

2013-10-09c-e-66-opt.png
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)

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