A pulsed 931‐A photomultiplier and TW‐10 traveling wave oscilloscope have been used to measure the scintillation decay times of (a) transtilbene, (b) terphenyl‐in‐toluene, and (c) polystyrene plastic containing one percent terphenyl, 0.03% α‐NPO, and 0.01% zinc stearate. The times for 1/e decay are (a) 4±1×10−9 sec, (b) 2.2±0.3×10−9 sec, and (c) 2.2±0.3×10−9 sec. The behavior of the multiplier with large collector currents was studied, using a synchronized flash lamp. Linear currents up to 1.5 amperes and maximum currents up to 15 amperes were obtained. Currents in the ampere range can give rise to an oscillation which may limit the application of pulsed photomultipliers.
REFERENCES
1.
2.
Ben Petree and Frank Viera, Jr., “A study of the performance of photomultipliers operated at high voltage,” Natl. Bur. Standards Report 2065.
3.
J. S. Allen and T. Engelder, “Rise and decay times of pulses from photomultiplier tubes using liquid phosphors,” AECU‐996, LADC‐871.
4.
A more complete description of the decay time measurements is given by S. Singer, “Measurement of rise and decay times of three fast scintillators including a special plastic,” LASL Report 1694.
5.
The specific resistor values were chosen by letting for for ( corresponds to the photocathode—1st dynode resistor).
6.
R. V. Talbot and L. M. Johnson, “The TW‐10: A high writing speed cathode ray tube with distributed deflection,” NRL Report 4377.
For information on the TW‐9, a predecessor of the TW‐10, see
Smith
, Talbot
, and Smith
, Proc. Inst. Radio Engr.
40
, 297
(1952
).7.
Cathode Ray tube Displays, MIT Radiation Laboratory Series, (McGraw‐Hill Book Company Inc., New York), Vol. 22, p. 290.
8.
Lawrence Arguimbau, Vacuum Tube Circuits (John Wiley and Sons, Inc., New York, 1948).
9.
Manufactured by Edgerton, Germeshausen, and Grier, Inc., Boston, Massachusetts.
10.
Since this work was carried out, further investigations of this effect was undertaken. It appears that the rms power developed during the “on” time of is almost 0.5 megawatt, very nearly equal to the peak power put into the system (10 000 v at 55 amp). A further description of this investigation will be published.
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© 1956 The American Institute of Physics.
1956
The American Institute of Physics
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