Difference between revisions of "September 12, 2011"

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|2359||Centered||In ||Open ||Out||No  
 
|2359||Centered||In ||Open ||Out||No  
 
|align="left"|Test radiator in/out
 
|align="left"|Test radiator in/out
R(upstream) = 157/40244 = 0.0039 e+/pulse
+
R(upstream) = 157/40244 = 0.0039 e+/pulse,<br> R(downstream) = 183/40244 = 0.0045 e+/pulse
 
 
R(downstream) = 183/40244 = 0.0045 e+/pulse
 
 
|-
 
|-
 
|2360||Centered||In ||Open ||Centered||No  
 
|2360||Centered||In ||Open ||Centered||No  
 
|align="left"|Test radiator in/out
 
|align="left"|Test radiator in/out
R(upstream) = 898/40244 = 0.022 e+/pulse
+
R(upstream) = 898/40244 = 0.0223 e+/pulse,<br> R(downstream) = 1040/40244 = 0.0258 e+/pulse
 
+
<span style="color:red">About 83% of photons are coming from the radiator. Bad</span>
R(downstream) = 1040/40244 = 0.026 e+/pulse
 
 
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Revision as of 15:02, 12 September 2011

go back

summary what was been done

Run # Beam Dump magnet Collimator Radiator 10 um Al Target Comments
2359 Centered In Open Out No Test radiator in/out

R(upstream) = 157/40244 = 0.0039 e+/pulse,
R(downstream) = 183/40244 = 0.0045 e+/pulse

2360 Centered In Open Centered No Test radiator in/out

R(upstream) = 898/40244 = 0.0223 e+/pulse,
R(downstream) = 1040/40244 = 0.0258 e+/pulse About 83% of photons are coming from the radiator. Bad