QADC spectrum

QDC Analysis

details proving signal is from detector ON/OFF

details of measuring shutter OPEN - Closed (why negative counts????)

The first test for the detector signal after installing U-233 is by using CAEN V792 Q-ADC (Analog charge to digital converter). The aim of this test is to test the shutter ability to help in distinguishing the emitted particles from U-233 source based on liberated charge from their ionization in gas.

charge collected as the voltage is 2.60 2.90 kV for GEM and cathode successively

charge collected as the voltage is 2.65 2.95 kV for GEM and cathode successively

charge collected as the voltage is 2.70 3.00 kV for GEM and cathode successively

charge collected as the voltage is 2.75 3.05 kV for GEM and cathode successively

charge collected as the voltage is 2.80 3.10 kV for GEM and cathode successively

charge collected as the voltage is 2.60 2.90 kV for GEM and cathode successively

charge collected as the voltage is 2.65 2.95 kV for GEM and cathode successively

charge collected as the voltage is 2.70 3.00 kV for GEM and cathode successively

charge collected as the voltage is 2.75 3.05 kV for GEM and cathode successively

charge collected as the voltage is 2.80 3.10 kV for GEM and cathode successively

A Non-linear increase in the charge collected by the Q-ADC as the voltage increases for GEM HV-circuit, also the figures show the change in the charge spectrum as the shutter position changed, shutter open's charge spectra show more collected charge than that of shutter close.

GEM voltage vs. the charge of the peaks appear as the shutter is open (blue, green) and close (red)

GEM voltage vs. the reltive gain of the peaks appear as the shutter is open (blue,green)and close(red)

First Peak in Shutter open spect

voltage (kV)	channel number for three runs	charge calibration factor	Charge (nC)	Average Charge from the figure (nC)
2.75	1143+_3 ,1274+_3 , 1026+_3	0.0393	45.11	50
2.80	1078+_2, 1015+_2, 1110+_1	0.051	54.45	50

The table above shows a comparison between the averaging 3 charge spectra to find the channel number for the first peak as the shutter is open (last column), and a gaussian fitting for each peak for each run separately to find the average, then calculating the average for the three peaks' channel number (column 3). The comparison shows that the first peak is still considered saturated.

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