
2
,
C
Q
V=
,
)(
sin
sin RRR RRR
R++ +
=∠
∠
τ
3. INSTALLATION INSTRUCTIONS
3.1. CONNECTION TO
PHOTOMULTIPLIER TUBE
Connect the output of the photomultiplier to the
input of the 113 with a coaxial cable. This cable
should be kept as short as practicable. The
photomultiplier outputcanbetakenfrom the anode,
cathode, or any dynode and will generally be ac-
coupled. The input connector of the 113 is isolated
for 1000 V dc; however, it can be modified for
3000-V dc isolation by being replaced with a type
SHV connector.
3.2. CONNECTION TO A SHAPING MAIN
AMPLIFIER
The 113 can be used to drive long lengths of 93
S
cable to a shaping amplifier and is designed to be
directly compatible with ORTEC transistor main
amplifiers. The output impedance of the 113 is
93
S
; therefore if the 93
S
cable is used, it is not
necessary to terminate it at the receiving end. If
unterminated cable is used on the output, with
impedance other than 93
S
, resistor R24 should be
adjusted for an output impedance equal to the
value of the cable impedance to prevent pulse
reflections.
3.3. INPUT POWER
Power for the 113 is supplied through an Amphenol
connector (17-20090) on the rear of the chassis.
Power may be supplied by a single 45-V battery
with a tap at 22.5 V (use the tap as ground,
providing +22.5 V and
!
22.5 V; current drain is 17
mA)orbyanywell-filtered±24-Vpowersupplysuch
as the ORTEC 114 Preamplifier Power Supply.
If the 113 is used with ORTEC transistor main
amplifiers, power for the preamplifier can be
supplied from the main amplifier through the
interconnecting cable supplied with the 113.
3.4. TEST PULSE
A voltage pulse can be inserted at the Test Pulse
connector on the rear of the 113. The 113 has a
built-in charge terminator that converts the input
voltage to an input charge to simulate a charge
pulse from the photomultiplier tube. The shape of
the voltage test pulse should have a fast rise time
(less than 10-8 sec) followed by a slow expoential
decay back to the baseline (2 to 4 X 10-4 sec). A 1-V
input signal at the Test Pulse connector produces a
pulse of approximately 135 mV when an input
capacity of 100 pF is selected by S1.
4. OPERATING INSTRUCTIONS
The shape of the output pulse from the
photomultiplier tubeisdependent onthe form of the
light pulse, the transit-time spread in the
photomultiplier, and the anode resistance and
capacitance. Since the form of the light pulse and
the transit time of the tube cannot be altered, our
concern is with the anode and associated circuitry.
The signal at the anode appears as a current pulse
or a quantity of charge, and the voltage produced
by this quantity of charge is given by
where C = Cs+ Cin (see Fig. 4.1). (C1and C2are
coupling capacitors that are large in value
compared to C, and therefore accumulate a
negligible amount of voltage from the charge
transferred.) The voltage developed acrossCs+ Cin
will decay with a time constant of
J
f= R
J
C, where
and Rs= high-voltage supply output resistance.