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  1. "Photoelectric Properties of Thin Films of Alkali Metal," Ives, Astrophysical J., 60, No. 4, November 1924.
  2. "Electrical and Photoelectric Properties of Thin Films of Rubidium on Glass," Ives and Johnsrud, Astrophysical J., 62, p. 309; 1925.
  3. "Plane Waves of Light," Fry, to appear in J.O.S.A. & R.S.I., 16, January, 1928.
  4. The values for the constants of rubidium as here determined differ considerably from those obtained by Natnanson (Phys. Rev., 40, 3, p. 231) who made his observations on a rubidium-backed glass plate. He gives (interpolating for λ5461),n= .14, and nk (our Ko) 1.15.
  5. See a résumé on "Atomic Dimensions" by Lunnon, Phys. Soc. London, p. 93, Feb. 15, 1926.
  6. The constants chosen for platinum may be compared with those obtained by W. Meier (Ann. d. Phys., 31, p. 1064; 1910). He gives n=2.44 and nk (our K0) 3.44.

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"Photoelectric Properties of Thin Films of Alkali Metal," Ives, Astrophysical J., 60, No. 4, November 1924.

"Electrical and Photoelectric Properties of Thin Films of Rubidium on Glass," Ives and Johnsrud, Astrophysical J., 62, p. 309; 1925.

"Plane Waves of Light," Fry, to appear in J.O.S.A. & R.S.I., 16, January, 1928.

The values for the constants of rubidium as here determined differ considerably from those obtained by Natnanson (Phys. Rev., 40, 3, p. 231) who made his observations on a rubidium-backed glass plate. He gives (interpolating for λ5461),n= .14, and nk (our Ko) 1.15.

See a résumé on "Atomic Dimensions" by Lunnon, Phys. Soc. London, p. 93, Feb. 15, 1926.

The constants chosen for platinum may be compared with those obtained by W. Meier (Ann. d. Phys., 31, p. 1064; 1910). He gives n=2.44 and nk (our K0) 3.44.

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