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
| Run # | Run Duration (s) | Configuration | 
| 6488 | min  s | 2->60Hz rep rate, Looking at NaI in shielded cell at -600 Volts,  Magnet on Accelerator side deflects electrons, Tungsten target is out, triggering only on the beam gate and looking at ADC channel 3 | 
| 6489 | min  s | same as above except: 120Hz rep rate, -500 Volts, | 
| 6490 | min  s | same as above except: -550 Volts, | 
| 6491 | min  s | same as above except: -575 Volts, | 
| 6492 | min  s | same as above except: inserted Aluminum brick to be sure electrons are staying on accelerator side,  drops NaI output by factor of 2 | 
| 6493 | min  s | same as above except: -600 Volts | 
| 6494 | min  s | same as above except: -700 Volts | 
| 6498 | min  s | same as above except: -500 Volts, magnet out | 
| 6499 | min  s | same as above except: -700 Volts, very similar ADC spectrum for magnet in | 
| 6500 | min  s  (54420 , 120 Hz pulses =453.5 sec) | same as above except: removed Al brick beam stop, increased current from zero until signal was observed in experimental cell NaI (probably mostly dark current from RF cavity) | 
| 6501 | min  s (54297 pulses) | same as above except: inserted Al brick beam stop,   | 
| 6502 | min  s (54297 pulses) | same as above except: REmoved Al brick beam stop | 
40 MeV on Tungsten
40 MeV electrons are hitting the positron production Tungsten target
| Run # | Run Duration (s) | Configuration | 
| 6503 | 3 min 46  s ( pulses) | Dipoles in positron mode. Al Brick in along 8 inch length | 
| 6504 | min  s ( pulses) | same as previous run, Al brick OUT | 
| 6505 | min  s ( pulses) | same as previous run, Dipoles in Electron mode,   | 
| 6506 | min  s ( pulses) | same as previous run, Selection Magnet bending electrons up positioned after 50 micron Ti vacuum window,   | 
| 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, | 
Shielded Cell direct beam with magnet
reconfigure with sweep magnet in shielded cell to deflect charged particles towards NaI detector #3,
| 6511 | min  s ( pulses) | dipoles in electron mode transporting 8 MeV, NaI at -700 Volts | 
| 6512 | min  s ( pulses) | dipoles in electron mode transporting 6 MeV, Magnet is OUT | 
| 6513 | min  s ( pulses) | dipoles in electron mode transporting 6 MeV, Magnet is IN and deflecting positrons towards NaI | 
| 6514 | 12  min  3 s ( pulses) | same as last run except: dipoles in positron mode, doubled current from last run | 
| 6515 | min  s ( pulses) | same as last run except: positron dipoles set to 8 MeV, increased current and rep rate (150 Hz) | 
| 6516 | min  s ( pulses) | same as last run except: positron dipoles set to 6 MeV, | 
| 6517 | 2  min 18 s ( pulses) | same as last run except: Magnet is out | 
| 6518 | 7 min  10s ( pulses) | same as last run except: positron dipoles set to 8 MeV, sweep Magnet is out | 
| 6519 | min  s ( pulses) | same as last run except: sweep Magnet is In positron bending mode | 
| 6520 | min  s ( pulses) | same as last run except: sweep Magnet is In electron bending mode | 
| 6521 | min  s ( pulses) | same as last run except: dipoles set to electron mode | 
38 MeV electrons with 859 pVs/50 Ohms per 100 nsec wide pulse
a scope measurement of the 38 MeV electron pulse impinging the tungsten target suggested that one pulse had
[math]\frac{0.859 \times 10^{-9} V s}{50 Ohm} = 1.7 \times 10^{-11} Coul \frac{1 e^-}{1.9 \times 10^{-19} Could} = 10^{8}[/math] electrons
or given the 100 nsec pulse width the peak current is
[math]\frac{1.7 \times 10^{-11} Coul}{100 \times 10^{-9} sec}[/math] = 0.017 Amps
I believe we need to run at 0.01 Amps to keep the ion pumps working.
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 | 
Positrons_Using_40Mev_Linac