EG&G ORTEC 474 Operating And Service Manual - Page 10
Browse online or download pdf Operating And Service Manual for Amplifier EG&G ORTEC 474. EG&G ORTEC 474 13 pages. Tinning filter amplifier
456
HIGHVOLTAGE
POWERSUPPLY
1-bv 1- in. KL236
459
DETECTOR
BIAS SUPPLY
265
PM
BASE
RCA
8575
PM
TUBE
Anode
11
SCINTIL
PREAMI
3
LATION
'LIFIER
1
r
460
OELAY-LINE
AMPLIFIER
473A
CONSTANT-
FRACTION
DISCRIMINATOR
^^Na Source
*
425A
NANOSECOND
DELAY
GeaO COAXIAL
DETECTOR
473A
CONSTANT-
FRACTION
DISCRIMINATOR
120-4
PREAMPLIFIER
474
TIMING
FILTER
AMPLIFIER
Start ^ f
^ Stop
TIMING SCA
457
TIME-TO
PULSE HEIGHT
CONVERTER
414A
FAST
COINCIDENCE
j
551
TIMING SCA
460
OELAY'LINE
AMPLIFIER
6240B
MULTICHANNEL
ANALYZER
8169
Fig. 7.1. Gamma-Gamma Coincidence System Using a Piastic Scintiilator and a Large
Ge(Li) Coaxial Detector.
uses a fast plastic scintiilator and the stop channel uses
a coaxial germanium detector. Excellent timing spectra
have been obtained by combining the pulse shaping avail
able with the 474 together with the use of the slow-rise-
time (SRT) reject circuitry in the constant-fraction dis
criminator. The SRT circuitry is most effective when used
with a wide dynamic range of energies. It can provide
dramatic improvement in timing resolution below the
FWHM level and makes reliable timing data possible at
even the FW(1/100)M level.
The SRT circuitry in the constant-fraction discriminator
can provide improved timing resolution by rejecting those
logic pulses that result from leading-edge timing in the
instrument. Since the input signals that cause leading-
edge walk represent valid energy information, use of the
SRT circuitry results in a loss in the counting efficiency of
the system.
A system for measuring the lifetimes of excited states at
extremely low energies is similar to the system shown in
Fig. 7.1. In this configuration the coaxial Ge(Li) detector
and preamplifier are replaced with a Ge(Li) low-energy
photon spectrometer (LEPS) detector and preamplifier.
7.3.
NANOSECOND FLUORESCENCE
SPECTROMETRY
The ORTEC 9200 Nanosecond Fluorescence Spectrom
eter is used in lifetime measurements of excited molecular
states. In the specific application where the molecular
structure is studied, the experimenter seeks to verify a
complex model of a particular molecule or to determine
how a particular molecule is altered by its surroundings.
This type of experiment requires that the total efficiency,
the exact energy, and the complete time function involved
in the de-excitation of an electronic state be known so that
the e,xperimental results can be fit precisely to a model.
Figure 7.2 shows the 9200 System, and Fig. 7.3 shows the
detailed lifetime characteristics of a 0.1 N solution of
quinine sulfate in sulfuric acid that was excited with im
pulses of light at approximately 340 nm with the 9200
System. The quantity of information available from such a
lifetime measurement is illustrated by this set of data.