Abstract

The spectral energy distribution of radiation from water bombarded by radium gamma-rays or P32 beta-rays is that expected for Cerenkov radiation. A solution of P32 in water furnishes a source of Cerenkov radiation which is convenient for the determination of the spectral sensitivity of photographic emulsions.

© 1953 Optical Society of America

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References

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  1. L. I. Schiff, Quantum Mechanics (McGraw-Hill Book Company, Inc., New York, 1949).
  2. G. B. Collins and V. G. Reiling, Phys. Rev. 54, 499 (1938).
    [Crossref]
  3. C. E. Kenneth Mees, The Theory of Photographic Process (Macmillan Company, New York, 1948).

1938 (1)

G. B. Collins and V. G. Reiling, Phys. Rev. 54, 499 (1938).
[Crossref]

Collins, G. B.

G. B. Collins and V. G. Reiling, Phys. Rev. 54, 499 (1938).
[Crossref]

Kenneth Mees, C. E.

C. E. Kenneth Mees, The Theory of Photographic Process (Macmillan Company, New York, 1948).

Reiling, V. G.

G. B. Collins and V. G. Reiling, Phys. Rev. 54, 499 (1938).
[Crossref]

Schiff, L. I.

L. I. Schiff, Quantum Mechanics (McGraw-Hill Book Company, Inc., New York, 1949).

Phys. Rev. (1)

G. B. Collins and V. G. Reiling, Phys. Rev. 54, 499 (1938).
[Crossref]

Other (2)

C. E. Kenneth Mees, The Theory of Photographic Process (Macmillan Company, New York, 1948).

L. I. Schiff, Quantum Mechanics (McGraw-Hill Book Company, Inc., New York, 1949).

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Tables (1)

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Table I

Equations (5)

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N = 2 π 137 ( 1 c 2 n 2 υ 2 ) d ν c .
N d ν ( d λ / λ 2 ) .
E 1 E 2 = d λ 1 d λ 2 ( λ 2 λ 1 ) 3 .
E = λ Δ λ λ + Δ λ E λ d λ = K λ Δ λ λ + Δ λ λ 3 d λ = K λ 3 L d ,
E 1 E 2 = ( λ 2 λ 1 ) 3 d 2 d 1 .