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28
INTERNATIONAL PROJECTIONIST
December 1933
(Left) FIG. 1 — P.E. characteristics of potassium-hydride caesium-oxygen-silver cells
and
(Beloiv) FIG. 2 — Effects on the photoelectric sensitivity of various thicknesses of the outer layer of caesium
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5°
. NORMAL N^'SURFACE
4.5 ATOM_A LAYERS \
\o.3 ATOM \ LAYER
4000 5000 6000 7000 8000 9000 10,000 11,000 12,000 WAVE-LENGTH IN ANGSTROM UNITS
7000 8000 9000 10,000 11,000
WAVE-LENGTH IN ANGSTROM UNITS
12,000
previously used. The relative response of the two types of cathodes to tungsten light of color temperature 2710° K over the spectral range from 3,000 to 11,000 Angstrom units is given in Figure 1.
To obtain a highly sensitive cathode surface, and one whose long wave-length limit extends so far into the infra-red, it is very essential that the residuum of caesium in excess of that necessary to combine with the silver oxide be held within extremely close limits. Studies have been made of the effect of additional amounts of caesium on the photosensitivity of the surface. In these studies the spectral response of a normally prepared surface has been obtained, and then additional caesium allowed to condense on the cathode surface at such a slow rate that the change in sensitivity of
the surface with added caesium coverage could be observed.
Effect of Added Caesium
Typical results of this kind are shown in Figure 2. From this figure it can be seen that the long wave-length limit recedes from about 12,000 A. to 9,600 A. by the addition of about 0.3 layer of caesium. When 4.5 layers have been added to the surface, the long wavelength limit has receded further to 8,400 A. The integrated area under each curve is proportional to the total sensitivity for that surface condition. For 0.3 of an atom layer added, the total
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sensitivity is reduced to 60% of its initial value, and for 4.5 layers it is further reduced to 25% of its initial value.
The 3A type photoelectric cell has been standardized for sound picture applications. Its cathode is of the caesium-oxygen-silver type. A still higher output is desired from this cell than the increased sensitivity of its cathode makes possible. To further increase the sensitivity, the cell is filled with argon to a pressure of a few hundredths of a millimeter of mercury. With anode potentials of less than 20 volts the behavior of the cell is identical with the high vacuum one. For anode potentials greater than 20 volts the anode current rises above that of the vacuum cell and diverges rapidly from it. At 90 volts potential the anode current is approxi
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