Difference between revisions of "September 13, 2011"
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R(beam down) = n/pulse<br> | R(beam down) = n/pulse<br> | ||
R(upstream) = e+/pulse<br> | R(upstream) = e+/pulse<br> | ||
− | <span style="color:red">About | + | <span style="color:red">About % of photons are coming from the radiator according to PS. Bad</span><br> |
− | <span style="color:red">About | + | <span style="color:red">About % of neutrons are coming from the radiator according to n detector down. Good</span> |
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Revision as of 15:35, 13 September 2011
summary what was been done
Run # | Beam | Dump magnet | Collimator | Radiator 10 um Al | Target | Comments |
---|---|---|---|---|---|---|
2385 | Up 2 mm | In | Open | Out | DU plate | Beam check-in run. Beam hardener off. DU plate 45/45 degree orientation and gammas hit the bottom right corner of plate from upstream view.
R(beam 45 left) = 6/173553 = 0.0000346 n/pulse |
2386 | Up 2 mm | In | Open | Up 2 mm | DU plate | Beam check-in run. 1" of Al hardener in front of upstream radiator.
R(beam 45 left) = n/pulse |
2387 | Up 2 mm | In | Open | Up 2 mm | DU plate | Lost beam |
2387 | Up 2 mm | In | Open | Up 2 mm | DU plate | Beam check-in run. Hardener in as before. Target realignment, now the gammas hit the center of DU plate, which is as before 45/45 degree orientation
R(beam 45 left) = n/pulse |