Super Clover Detector No 1

Super Clover Detector No 1

Enclosed are the files with the signal pictures acquired from the core channels of the
Segmented Super Clover 1 (the old one). The properties of the signals are given in the
following table:

Channel Rise Time Fall Time Undershoot Picture
1 (Red) 120 +/- 60 ns 85 +/- 15 mue s 2 +/- 1 % pulsshapei sc1_1_1 pulsshape sc1_1_2 pulsshape sc1_1_3 pulsshape sc1_1_4
2 (Blue) 120 +/- 60 ns 80 +/- 10 mue s 3 +/- 1.5 % pulsshapei sc1_2_1 pulsshape sc1_2_2 pulsshape sc1_2_3 pulsshape sc1_2_4
3 (Green) 130 +/- 70 ns 80 +/- 10 mue s 1.5 +/- 0.5 % pulsshapei sc1_3_1 pulsshape sc1_3_2 pulsshape sc1_3_3 pulsshape sc1_3_4
4 (Black) 120 +/- 60 ns 80 +/- 10 mue s 2 +/- 1 % pulsshapei sc1_4_1 pulsshape sc1_4_2 pulsshape sc1_4_3 pulsshape sc1_4_4

Polarity of the pulses is negative. The picture files are grouped in 4, each group corresponds
of one channel, described by the second digit in the file name; sc1_2_3 means ch.2. pic.3.
The four pictures of each channel are acquired at identical conditions and show different pulses.
The source used is 22-Na.

Please note the following:
- Since the rise time of the pulse (for the negative pulses this is fall time) is defined as the
time between 10% and 90% of the amplitude of the pulse, the different amplitude pulses
have different rise times. Therefore, the variations in the table are in the order of 50%.
- The rise time depends strongly on the physics of the interactions inside and those effects
affect the rise time and its variations.
- The fall time is fixed by circuitry of the preamplifier; however, noise contribution also
affects its determination.
- The pulses are aquired 'in situ', thus some reasonable ambient noise is also included.
Ivan Kojouharov

Super Clover Detector No 2