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More on Applications for the DB-2
The primary use of this pulse generator is to
simulate actual operating conditions without
requiring a live source and detector combination.
Such parameters as frequency response, linearity,
and discrimination levels may easily be measured
without the inconvenience of dim oscilloscope
display or long accumulation times. Proper operation
of baseline restorer circuits may be quickly
verified. Scalers and ratemeters may be checked for
satisfactory pulse recognition under random pulse
conditions.
The negligible amplitude shift with
frequency of the pulser makes the standard frequency
test using a live source and a low rate precision
pulse generator unnecessary.
Although most test applications
will find the pulser connected to the test input of
a charge sensitive preamplifier, it is possible to
simulate the preamp itself with the pulse generator.
The pulser is connected directly to the main
amplifier and the preamp decay time constant is
matched by proper selection of the pulser fall time.
Set up of a system containing an inaccessible preamp
can then be accomplished with ease.
For accurate simulation of detector
pulse shapes, the rise time control should be
adjusted to match 2.2 times the detector decay time
constant. For example, if a pulse shape analyzer
working with CsI-NaI phoswich is to be tested, the
pulse generator rise time should be set to 0.5 µsec
rise time for the NaI signal, and 2 µsec for the CsI
signal. Intermediate signals are best obtained by
mixing the outputs from two synchronized generators,
2 µsec rise time. By varying the amplitude ratio of
the two generators, intermediate values of rise time
are generated.
Solid state and plastic detectors
have decay constants far shorter than the adjustment
range of this generator. However, the shaping time
constants used in virtually all systems are greater
than the 100 nsec minimum rise time. The ballistic
deficit formula predicts the reduction in amplitude,
B. D., for a shaping system containing identical
time constants for all shaping.
B.D. = 
where n = the number of
integrations with time, constant =RC, and tr
is the rise time of the preamp output. The preamp
output rise time may be calculated from:
where tp is the pulser rise time and ti is the rise time of the preamp in response to a unit step of zero rise time. The ballistic deficit for a preamplifier with a ti of 10 nsec used with a shaping amplifier6 with 1 µsec time constants would be only 0.02% when used with this pulse generator. Therefore, the ballistic deficit caused by this pulser may be ignored for most applications.
The external reference allows remote programming of the amplitude of the pulser, and the external trigger permits control of the output pulse rate. The latter provision is especially convenient if the average random rate needs to be controlled and an external random clock is unavailable. By placing the pulser in the random mode, a periodic waveform at the external trigger input will control the average random rate.
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