Difference between revisions of "September 20, 2011"
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pulses<br> | pulses<br> | ||
R(bottom) = 0 n/pulse<br> | R(bottom) = 0 n/pulse<br> | ||
− | R(upstream) = 0. | + | R(upstream) = 0.000908 e+/pulse<br> |
− | <span style="color:red">About '''%''' of photons are coming from the radiator according to PS. Very Good</span><br> | + | <span style="color:red">About '''97%''' of photons are coming from the radiator according to PS. Very Good</span><br> |
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Revision as of 14:46, 20 September 2011
summary what was been done
- current 140 mA
- pulse width 2 us
- rep rate 180 Hz
- E = 25 MeV
Run # | Beam | Dump magnet | Collimator | add coll | Hardener 1" Al | Radiator 10 um Al | Target | Comments |
---|---|---|---|---|---|---|---|---|
2502 | Up 90A |
In | Open | In | Yes | In | DU cylinder | Test radiator in/out.
120664 pulses |
2503 | Up 90A |
In | Open | In | Yes | Out | DU cylinder | Test radiator in/out.
121258 pulses |
2504 | Down 86A |
In | Open | In | Yes | In | DU cylinder | Test radiator in/out.
R(bottom) = 0.00137 n/pulse -> ×180×60 = 14.8 n/min |
2505 | Down 86A |
In | Open | In | Yes | Out | DU cylinder | Test radiator in/out.
pulses |
Production runs
Run # | Beam | Dump magnet | Collimator | add coll | Hardener 1" Al | Radiator 10 um Al | Target | Comments |
---|---|---|---|---|---|---|---|---|
2494 | Up 90A |
In | Open | In | Yes | In | DU cylinder | Long production run
pulses |