Difference between revisions of "PePPO NaI PositronDetector 4 JLab"
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Revision as of 16:53, 24 March 2011
Detector setup for a NaI positron detector for PePPO
NaI detector
The PMT is powered by a HV supply which should have a DC ripple less than 200 mV peak-to-peak at 3kV/3mA. A DC ripple will change the gain of the PMT and cause the energy resolution to deteriorate.
The Linearity of the detector system is another way to reduce the energy resolution. The measured PMT output should be linear with the input signal when the gain is constant. This linearity can be measured using 2 radiation sources.
Input HV: +1085 V
Input Current: 2.362 mA
Running CODA: Running CODA
Measurements Using V792 QDC
Run 1979
Start Time : March 23:12:30:26
End Time: March 23: 13:10:47
Elapsed time: 2421 seconds
Run 1980
Remove Na-22 source from top of NaI crystal.
Start Time : March 23:13:11:23
End Time: March 23: 15:56:40
Elapsed Time:6317 seconds
Let's lower the gain of the Phillips 777 amplifier so the 511 peak is around channel 500. This way the 1 MeV photons may come on scale.
Run 1982
Overnight Cosmic Run
Start Time : March 23: 16:01:47
End Time: March 24: 09:41:31
Elapsed Time:63558 seconds
Run 1983
Start a run using Co-60
Start Time : March 24: 09:46:25
End Time: March 24: 10:14:24
Elapsed Time: 1679 seconds
The 1.x MeV gammas appear near channel 1200.
I'll do a long Na-22 run and think about upping the amplifier gain again to put the Co-60 peak around channel 3000.
The Co-60 source trigger rate is about 750 Hz and the Na-22 trigger rate was about 450 Hz.
Run 1984
Start a run using Na-22
Start Time : March 24: 10:16:49
End Time: March 24: 11:02:38
Elapsed Time: seconds
Gain
Linearity
Readout
F250
JLab's F250 flash ADC will be used to measure the NaI output
Na-22 source
North American Scientific Model CAL2600
Activity = 9.803 \muCi on 5/1/05
Serial Number 64236
Co-60 source
North American Scientific Model CAL2600
Activity = 9.641 \muCi on 5/1/05
Serial Number 64120