DocumentCode
386798
Title
High speed photomultipliers
Author
Miller, Ross ; Wittwer, N.
Author_Institution
Bell Telephone Laboratories, Inc., Murray Hill, NJ, USA
Volume
13
fYear
1966
fDate
21-25 March 1966
Firstpage
7
Lastpage
16
Abstract
Experimental results on two 8-stage photomultipliers exhibiting flat baseband response to
Gc will be discussed. One photomultiplier employs crossed electric and magnetic fields, the other is purely electrostatic. At present both devices employ Cu-Be dynodes and an internally situated, opaque-backed
photocathode. Frequency response measurements have used heterodyning between the modes of the Zeeman-split doppler profiles of a 6328 A He-Ne laser and also shot noise in the current from a steadily illuminated photocathode as sources of microwave modulated current. Both photomultipliers have been used to observe sub-nanosecond pulses from phase-locked He-Ne and argon ion lasers. An estimate of the frequency response to be expected from
identical stages of secondary emission, when only the secondary electron emission velocities contribute to electron transit time differences, gives results in agreement with experiment, assuming that the most probable secondary electron emission energy from BeO is about 3 e.v. This value is consistent with the direct measurements of others.
Gc will be discussed. One photomultiplier employs crossed electric and magnetic fields, the other is purely electrostatic. At present both devices employ Cu-Be dynodes and an internally situated, opaque-backed
photocathode. Frequency response measurements have used heterodyning between the modes of the Zeeman-split doppler profiles of a 6328 A He-Ne laser and also shot noise in the current from a steadily illuminated photocathode as sources of microwave modulated current. Both photomultipliers have been used to observe sub-nanosecond pulses from phase-locked He-Ne and argon ion lasers. An estimate of the frequency response to be expected from
identical stages of secondary emission, when only the secondary electron emission velocities contribute to electron transit time differences, gives results in agreement with experiment, assuming that the most probable secondary electron emission energy from BeO is about 3 e.v. This value is consistent with the direct measurements of others.Keywords
Baseband; Cathodes; Electron emission; Electrostatics; Frequency response; Laser modes; Laser noise; Magnetic field measurement; Masers; Photomultipliers;
fLanguage
English
Publisher
ieee
Conference_Titel
1958 IRE International Convention Record
Conference_Location
New York, NY, USA
Type
conf
DOI
10.1109/IRECON.1965.1147501
Filename
1147501
Link To Document