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Saturation Effects on the SVX Chip. Peter Hasiakos D0 test stand-May/Jun 2004. Purpose/motivation. Saturation loss of signal on subsequent pulse Potential issue for high occupancy channels in accelerator Goals: to verify occurrence of this phenomenon, and to quantify it.
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Saturation Effects on the SVX Chip Peter Hasiakos D0 test stand-May/Jun 2004
Purpose/motivation • Saturation loss of signal on subsequent pulse • Potential issue for high occupancy channels in accelerator • Goals: to verify occurrence of this phenomenon, and to quantify it
At the Test Stand… • 2 pulse generators trigger LED • Main pulse only sends 1 photon, so the early pulse makes the significant contribution to saturation • LED= light source (emulates photoelectric effect from collisions) • Photons VLPC SVX chip on AFE 1 board ADC counts • Sequencer, 1553 and VRB coordinate data • PC used to record, analyze (Poisson distributions)
Details on SVX Saturation Event (Photon detected) Event clock 1 crossing=396 ns Eventually, the Amount of charge (signal) levels off Q1 Q0 SVX Saturation
Timing issues * Data must be taken after this point (end of chip reset window)
Task #1:Observe how signal decays as previous pulse increases Pedestal (@ RAMPTRIM=350), mean=Po=41.8 main generator activated (early pulse off): mean=56.4
Task #1, Cont’d Main pulse held fixed, early pulse @ 8V, 20 nsec width: mean= 54.7 8V, 30 nsec width: mean=51.3
Task #1, cont’d 8 V, 40 nsec width: mean=44.3… a drastic decrease plots confirm hypothesis that signal decreases with increasing saturation
Task #1: Primary results -this plot shows reduction in ADC mean (of the late pulse) as early pulse width increases Relative signal= s/s0-1, where s is the mean ADC signal of main pulse and s0 corresponds to no early pulse. We will call the quantity s/s0 the loss fraction, L. -Next step: determine how much light is in the early pulse
Task #2: analyze amount of light in early pulse Pedestal (ramptrim @ 150--more light) Early pulse= 4 V, width=10 nsec
Task #2, cont’d @ 8 V; width=10 ns @ 8 V; width=30 ns
Determing number of pe’s for a given pulse of light We use the relationships N= /g N=(/)^2 * Calculated from Poisson distribution where =mean signal, N=number of pe’s, and g=gain, and =standard deviation
Task #2: Raw results N=(/)^2 Dependence on mean ADC signal necessity to investigate if saturation is STILL occurring in single pulse run
Problem: saturation also occurs with single, early pulse gain is calculated from and at varying amounts of light. Without saturation loss, gain=constant=g0 *We see that the gain drops ~10% at a width of 25 nsec (about 15 pe’s).
Correcting the problem -correct valid calculations of N -because early pulse is the significant cause of saturation, we can use the same loss fraction, L, from Task 1 -Task 1 also indicated that before 10 pe’s, the gain stays at the value g0 and is unaffected by saturation ’= /L and N’= ’/ g0 Final result: corrected number of photons for each early pulse of light
Final Results • In sum, we have used task 1 to find the magnitude of saturation effect, and task 2 to rescale in terms of #pe • After an arrival of ~10 pe’s, there is a 10% loss in signal • After an arrival of ~20 pe’s, there is a 30% loss in signal
Conclusions • New test stand is working • SVX chip only gives correct results in proper time window • Results indicate that noticeable saturation effects begin occurring after a previous signal of ~10-15 pe’s