Difference between revisions of "September 16, 2011"

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R(upstream) = 1053/160876 = 0.0065 e+/pulse<br>
 
R(upstream) = 1053/160876 = 0.0065 e+/pulse<br>
 
|-
 
|-
|<span style="color:blue">'''2466'''</span>||Down<br> 86A||In ||Open ||Yes ||Down||Out
+
|<span style="color:blue">'''2466'''</span>||Down<br> 86A||In ||Open ||Yes ||Down||DU cylinder
 
|align="left"|<span style="color:blue">'''Long production run'''</span>
 
|align="left"|<span style="color:blue">'''Long production run'''</span>
 
R(beam down) = 243/972019 = 0.00025 n/pulse <span style="color:red"> -> ×180×60 = '''2.7 n/min'''</span><br>
 
R(beam down) = 243/972019 = 0.00025 n/pulse <span style="color:red"> -> ×180×60 = '''2.7 n/min'''</span><br>
 
R(upstream) =  0.0064 e+/pulse<br>
 
R(upstream) =  0.0064 e+/pulse<br>
 
|-
 
|-
|<span style="color:blue">'''2467'''</span>||Up<br> 90A||In ||Open ||Yes ||Up||Out
+
|<span style="color:blue">'''2467'''</span>||Up<br> 90A||In ||Open ||Yes ||Up||DU cylinder
 
|align="left"|<span style="color:blue">'''Long production run'''</span>
 
|align="left"|<span style="color:blue">'''Long production run'''</span>
 
R(beam down) = 292/972017 = 0.0003 n/pulse <span style="color:red"> -> ×180×60 = ''' 3.2 n/min'''</span><br>
 
R(beam down) = 292/972017 = 0.0003 n/pulse <span style="color:red"> -> ×180×60 = ''' 3.2 n/min'''</span><br>
 
R(upstream) =  0.00656 e+/pulse<br>
 
R(upstream) =  0.00656 e+/pulse<br>
 
|-
 
|-
|<span style="color:blue">'''2468'''</span>||Up<br> 90A||In ||Open ||Yes ||Up||Out
+
|<span style="color:blue">'''2468'''</span>||Up<br> 90A||In ||Open ||Yes ||Up||DU cylinder
 
|align="left"|<span style="color:blue">'''Long production run'''</span>
 
|align="left"|<span style="color:blue">'''Long production run'''</span>
 
R(beam down) = 0/162265 = 0 n/pulse <span style="color:red"> -> ×180×60 = ''' 0 n/min'''</span><br>
 
R(beam down) = 0/162265 = 0 n/pulse <span style="color:red"> -> ×180×60 = ''' 0 n/min'''</span><br>

Revision as of 20:27, 16 September 2011

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summary what was been done

Run # Beam Dump magnet Collimator Hardener Radiator 25 um Al Target Comments
2459 Up
90A
In Open Yes Out DU cylinder Beam check-in run.

R(beam down) = 1/160279 = 0.0000062 n/pulse
R(upstream) = 124/160279 = 0.00077 = e+/pulse

2460 Down
86A
In Open Yes Out DU cylinder Beam check-in run.

R(beam down) = 0/160873 = 0 n/pulse
R(upstream) = 142/160873 = 0.00088 = e+/pulse

2461 Down
86A
In Open Yes Down DU cylinder Beam check-in run.

R(beam down) = 33/160084 = 0.0002061 n/pulse -> ×180×60 = 2.2 n/min
R(upstream) = 990/160084 = 0.00618 e+/pulse
About 86% of photons are coming from the radiator according to PS. Good

2462 Up
90A
In Open Yes Up DU cylinder Beam check-in run.

R(beam down) = 0.000362 n/pulse -> ×180×60 = 3.9 n/min
R(upstream) = 1064/165434 = 0.00643 e+/pulse
About 88% of photons are coming from the radiator according to PS. Good

2463 Up
90A
In Open Yes Up Out Beam check-in run.

R(beam down) = 0 n/pulse
R(upstream) = 0.0062 e+/pulse

2464 Down
86A
In Open Yes Down Out Beam check-in run. Short beam off

R(beam down) = 0.000029 n/pulse
R(upstream) = 0.0055 e+/pulse

2465 Down
86A
In Open Yes Down Out Beam check-in run. Redoing 2464

R(beam down) = 3/160876 = 0.000019 n/pulse
R(upstream) = 1053/160876 = 0.0065 e+/pulse

2466 Down
86A
In Open Yes Down DU cylinder Long production run

R(beam down) = 243/972019 = 0.00025 n/pulse -> ×180×60 = 2.7 n/min
R(upstream) = 0.0064 e+/pulse

2467 Up
90A
In Open Yes Up DU cylinder Long production run

R(beam down) = 292/972017 = 0.0003 n/pulse -> ×180×60 = 3.2 n/min
R(upstream) = 0.00656 e+/pulse

2468 Up
90A
In Open Yes Up DU cylinder Long production run

R(beam down) = 0/162265 = 0 n/pulse -> ×180×60 = 0 n/min
R(upstream) = a/162265 = 0.0017 e+/pulse


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