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Dr. James Madsen
james.madsen@uwrf.edu
125 Centennial Science Hall
522 S. Sixth Street
Mail: 410 S. Third Street
River Falls, WI 54022

(715) 425-3235
Fax (715) 425-0652

 

O.M. Signals, Compared Over Varying Inputs

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Introduction

Here we set up a series of trials where we varied the input voltage to the O.M. to study its effect on signal shape and size.

Equipment:

Optical Module
Hamamatsu BB-7250, containing PMT model R5912-02
Oscilloscope
Lecroy Wavepro 7000
Photo Multiplier Tube
Hamamatsu R7081-10
Amanda type scintillater/P.M.T. box


Setup

The O.M. and the P.M.T were placed inside the dark box with their faces to a scintillater plate (the type in the Amanda type scintillater/P.M.T. box). The Amanda type scintillater/P.M.T. box was placed on top of the dark box, directly above the scintillater plate. The trigger on the Oscilloscope was set to qualify a trigger by the signal on the Amanda type scintillater/P.M.T. box to reach -30 mV, and the signal on the P.M.T. to reach -250 mV within 100 ns of the first. This setup was used to guarantee muon caused triggers. The signal from the O.M. was averaged and stored. Persistence recordings of all of the signals and histograms of the signal size were also recorded.

Results

Here is a normalized (by deviding by the highest value) comparison of the different average signals. There is a clear widening of the average signal as the input voltage increases. To explain this it is helpful the look at the persistence recording of the signals that were averaged (here). The large amount of wild noise that is down and to the right of the real signal pulse has the effect of pulling the average towards itself. The noise is probably caused by saturation of the O.M. as it is running at a high input voltage and is facing a scintillater plate that emits much more like per muon than a tank of water would.

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