Difference between revisions of "September 9, 2011"
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{| border="1" cellspacing="0" style="text-align: center; width: 1000px " | {| border="1" cellspacing="0" style="text-align: center; width: 1000px " | ||
| − | ! scope="col" width=" | + | ! scope="col" width="8%" | Run # |
| − | ! scope="col" width=" | + | ! scope="col" width="8%" | Beam |
| − | ! scope="col" width=" | + | ! scope="col" width="8%" | Dump magnet |
| − | ! scope="col" width=" | + | ! scope="col" width="8%" | Collimator |
| − | ! scope="col" width=" | + | ! scope="col" width="8%" | Radiator 10 um Al |
| − | ! scope="col" width=" | + | ! scope="col" width="8%" | Target |
| − | ! scope="col" width=" | + | ! scope="col" width="52%" | Comments |
|- | |- | ||
|2339||Up 2 mm||In ||Open ||Up 2 mm||No ||align="left"|'''R(upstr) = 2648/35092 = 0.075 e+/pulse''',\newline '''R(downstr) = 3191/35092 = 0.091 e+/pulse''' | |2339||Up 2 mm||In ||Open ||Up 2 mm||No ||align="left"|'''R(upstr) = 2648/35092 = 0.075 e+/pulse''',\newline '''R(downstr) = 3191/35092 = 0.091 e+/pulse''' | ||
Revision as of 19:03, 9 September 2011
summary what was been done
| Run # | Beam | Dump magnet | Collimator | Radiator 10 um Al | Target | Comments |
|---|---|---|---|---|---|---|
| 2339 | Up 2 mm | In | Open | Up 2 mm | No | R(upstr) = 2648/35092 = 0.075 e+/pulse,\newline R(downstr) = 3191/35092 = 0.091 e+/pulse |
| 2341 | Up 2 mm | In | Open | Out | No | R(upstream) = 1088/35494 = 0.031 e+/pulse, R(downstream) = 1328/35494 = 0.037 e+/pulse. About 59% of photons are coming from the radiator. Bad |
| 2342 | Down 2 mm | In | Open | Out | No | R(upstream) = 1586/36678 = 0.043 e+/pulse, R(downstream) = 1888/36678 = 0.051 e+/pulse. |
| 2343 | Down 2 mm | In | Open | Down 2 mm | No | R(upstream) = 2232/35488 = 0.063 e+/pulse. About 32% of photons are coming from the radiator. Bad |
| 2344 | Centered | In | Open | Centered | No | R(upstream) = 2683/35095 = 0.076 e+/pulse. |
| 2345 | Centered | In | Open | Out | No | R(upstream) = 1039/35094 = 0.029 e+/pulse. About 62% of photons are coming from the radiator. Bad |
| 2346 | Centered | In | Open | Out | No | PS Rate is: R(upstream) = 1286/35885 = 0.036 e+/pulse. Improved shielding around dump. |
| Based on the previous results the beam is total crap, so beam turn up. | ||||||
| 2349 | Centered | In | Open | Out | No | PS Rate is: R(upstream) = 404/35489 = 0.011 e+/pulse. |
| 2350 | Centered | In | Open | Out | No | PS Rate is: R(upstream) = 428/35093 = 0.012 e+/pulse. Additional shielding around the vacuum window of the beam pipe. |
| 2351 | Centered | In | Open | Centered | No | PS Rate is: R(upstream) = 1314/35094 = 0.037 e+/pulse. Additional shielding around the vacuum window of the beam pipe is removed. About 68% of photons are coming from the radiator. Still bad |
| 2352 | Up 2 mm | In | Open | Up 2 mm | D2O buttle | Asymmetry production run. About 40 min |
| 2353 | Up 2 mm | In | Open | Out | D2O buttle | plan About 30 min. |
Beam Realignment
Screen shot using Phosphorous screen
Electron beam on glass
12pm upstream view screen
12pm downstream view screen
