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References

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  1. F. C. Brown, Phys. Rev. 4, 85 (1914).
    [Crossref]
  2. L. A. Jones, J. O. S. A. 16, 259 (1928).
    [Crossref]
  3. Holmes and Whitman, Phys. Rev. 47, 337A (1935).

1935 (1)

Holmes and Whitman, Phys. Rev. 47, 337A (1935).

1928 (1)

L. A. Jones, J. O. S. A. 16, 259 (1928).
[Crossref]

1914 (1)

F. C. Brown, Phys. Rev. 4, 85 (1914).
[Crossref]

Brown, F. C.

F. C. Brown, Phys. Rev. 4, 85 (1914).
[Crossref]

Holmes,

Holmes and Whitman, Phys. Rev. 47, 337A (1935).

Jones, L. A.

L. A. Jones, J. O. S. A. 16, 259 (1928).
[Crossref]

Whitman,

Holmes and Whitman, Phys. Rev. 47, 337A (1935).

J. O. S. A. (1)

L. A. Jones, J. O. S. A. 16, 259 (1928).
[Crossref]

Phys. Rev. (2)

Holmes and Whitman, Phys. Rev. 47, 337A (1935).

F. C. Brown, Phys. Rev. 4, 85 (1914).
[Crossref]

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Figures (4)

F. 1
F. 1

Current, I, and e.m.f., E, from selenium crystal photo-e.m.f. cell for various illuminations.

F. 2
F. 2

Current, I, and e.m.f., E, from selenium crystal photo-e.m.f. cell for various wave-lengths using an equal energy spectrum.

F. 3
F. 3

Resistance, R, of selenium crystal photo-e.m.f. cell using an outside source of e.m.f. Quotient E/I where E and I are values shown in Fig. 1.

F. 4
F. 4

(a). Representing the granules of platinum making poor contacts with the surface of the selenium crystal. (b) A simplified and diagrammatic representation of the divided circuit of the photo-e.m.f. cell. This figure shows electron current directions.

Equations (1)

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I = k L ( R + R ) / ( R 1 + R 2 + R + 2 R ) .