Difference between revisions of "PosRun 10 14 2013"
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| 6507 || min s ( pulses) || same as previous run, dipoles set to positron mode and selection magnet rotated 180 degrees so positrons bend up, | | 6507 || min s ( pulses) || same as previous run, dipoles set to positron mode and selection magnet rotated 180 degrees so positrons bend up, | ||
+ | |- | ||
+ | | 6508 || min s ( pulses) || same as previous run:increase voltage from -700 to -850 | ||
+ | |- | ||
+ | | 6509 || min s ( pulses) || same as previous run, installed 2" thick graphite hardener | ||
+ | |- | ||
+ | | 6510 || min s ( pulses) || same as previous run, removed graphite hardener and selection magnet, returned to dipoles in electron mode, | ||
|} | |} | ||
Revision as of 21:12, 14 October 2013
Run list
Scaler channel #2 counts the number of beam pulses
Detector 4 is Beam Left and in ADC channel 7, Ortec Dual Spec amp set to course=10, fine=39, Canberra CFD set to 85 mV lower threshold
Detector 1 is Beam Right and in ADC channel 3, Ortec Dual Spec amp set to course=20, fine=10, Canberra CFD set to 70 mV lower threshold
In-flight
40 MeV on Tungsten
40 MeV electrons are hitting the positron production Tungsten target
FC -vs- 90A beam stop correlation
FC = Aluminum brick 2" from exit window near NaI detectors
50 Ohm scope termination
90 A BS (nVs) | FC (nVs) |
47 | 25 |
24 | 11.9 |
13 | 6 |
6.1 | 2.3 |
4.8 | 1.8 |