Difference between revisions of "September 19, 2011"
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R(upstream) = 0.00080 = e+/pulse<br> | R(upstream) = 0.00080 = e+/pulse<br> | ||
<span style="color:red">About '''93%''' of photons are coming from the radiator according to PS. Good</span><br> | <span style="color:red">About '''93%''' of photons are coming from the radiator according to PS. Good</span><br> | ||
| + | |- | ||
| + | |} | ||
| + | |||
| + | |||
| + | Good beam, good turning. So there are <span style="color:blue">'''2492'''production runs</span> | ||
| + | |||
| + | {| border="1" cellspacing="0" style="text-align: center; width: 1000px " | ||
| + | ! scope="col" width="7.2%" | Run # | ||
| + | ! scope="col" width="7.2%" | Beam | ||
| + | ! scope="col" width="7.2%" | Dump magnet | ||
| + | ! scope="col" width="7.2%" | Collimator | ||
| + | ! scope="col" width="7.2%" | Hardener 1" Al | ||
| + | ! scope="col" width="7.2%" | Radiator 10 um Al | ||
| + | ! scope="col" width="7.2%" | Target | ||
| + | ! scope="col" width="56.6%" | Comments | ||
| + | |- | ||
| + | |<span style="color:blue">'''2494'''</span>||Up<br> 90A||In ||Open ||Yes ||In||DU cylinder | ||
| + | |align="left"|Additional collimator in. '''Long production run'''</span> | ||
| + | 190006 pulses | ||
| + | R(beam down) = 0.00063 n/pulse <span style="color:blue"> -> ×180×60 = '''6.8 n/min'''</span><br> | ||
| + | R(upstream) = 0.0142 = e+/pulse<br> | ||
| + | |- | ||
| + | |<span style="color:blue">'''2494'''</span>||Up<br> 90A||In ||Open ||Yes ||In||DU cylinder | ||
| + | |align="left"|Additional collimator in. '''Long production run'''</span> | ||
| + | 190006 pulses | ||
| + | R(beam down) = 0.00063 n/pulse <span style="color:blue"> -> ×180×60 = '''6.8 n/min'''</span><br> | ||
| + | R(upstream) = 0.0142 = e+/pulse<br> | ||
| + | |- | ||
| + | |<span style="color:blue">'''2494'''</span>||Up<br> 90A||In ||Open ||Yes ||In||DU cylinder | ||
| + | |align="left"|Additional collimator in. '''Long production run'''</span> | ||
| + | 190006 pulses | ||
| + | R(beam down) = 0.00063 n/pulse <span style="color:blue"> -> ×180×60 = '''6.8 n/min'''</span><br> | ||
| + | R(upstream) = 0.0142 = e+/pulse<br> | ||
|- | |- | ||
Revision as of 00:04, 20 September 2011
Summary of the day
- current 120 mA
- pulse width 2 us
- rep rate 180 Hz
- E = 25 MeV
| Run # | Beam | Dump magnet | Collimator | Hardener 1" Al | Radiator 10 um Al | Target | Comments |
|---|---|---|---|---|---|---|---|
| 2479 | Up 90A |
In | Open | Yes | In | DU cylinder | Beam check-in run. Additional collimator in
R(beam down) = 0.000689 n/pulse |
| 2480 | Up 90A |
In | Open | Yes | Out | DU cylinder | Beam check-in run.
R(beam down) = 0.000018 n/pulse |
| 2482 | Down 86A |
In | Open | Yes | In | DU cylinder | Beam check-in run.
R(beam down) = 0.000717 n/pulse |
| 2483 | Down 86A |
In | Open | Yes | Out | DU cylinder | Beam check-in run. Beam lost.
R(beam down) n/pulse |
- current 160 mA
- rep rate 180 Hz
| Run # | Beam | Dump magnet | Collimator | Hardener 1" Al | Radiator 10 um Al | Target | Comments |
|---|---|---|---|---|---|---|---|
| 2488 | Down 86A |
In | Open | Yes | Out | DU cylinder | Beam returned without VS. Beam check-in run. Additional collimator in
R(beam down) = 0 n/pulse |
| 2489 | Down 86A |
In | Open | Yes | In | DU cylinder | Beam check-in run.
R(beam down) = 0.00057 n/pulse |
| 2490 | Up 90A |
In | Open | Yes | In | DU cylinder | Beam off. |
| 2491 | Up 90A |
In | Open | Yes | In | DU cylinder | Beam check-in run.
R(beam down) = 0.000569 n/pulse |
| 2492 | Up 90A |
In | Open | Yes | Out | DU cylinder | Beam check-in run.
R(beam down) = 0 n/pulse |
Good beam, good turning. So there are 2492production runs
| Run # | Beam | Dump magnet | Collimator | Hardener 1" Al | Radiator 10 um Al | Target | Comments |
|---|---|---|---|---|---|---|---|
| 2494 | Up 90A |
In | Open | Yes | In | DU cylinder | Additional collimator in. Long production run
190006 pulses
R(beam down) = 0.00063 n/pulse -> ×180×60 = 6.8 n/min |
| 2494 | Up 90A |
In | Open | Yes | In | DU cylinder | Additional collimator in. Long production run
190006 pulses
R(beam down) = 0.00063 n/pulse -> ×180×60 = 6.8 n/min |
| 2494 | Up 90A |
In | Open | Yes | In | DU cylinder | Additional collimator in. Long production run
190006 pulses
R(beam down) = 0.00063 n/pulse -> ×180×60 = 6.8 n/min |