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  1. Proc. Nat. Acad. Sciences, 2, p. 683; 1916.
  2. Phys. Rev., 17, p. 7; 1921.
  3. Taken from C. F. Hills curve Fig. 3 for a temperature of 26.3°C; Phys. Rev., 20, p. 265; 1922.
  4. The ion current of .5 divisions with liquid air on the trap is probably due entirely to the steady evolution of gas from the walls of the ionization gauge.
  5. Wright in The American Journal of Scicnce, 13, p. 49; 1877, probably had a large surface of gold compared to the rate of diffusion of the mercury vapor. The chances are, too, that the spectrum of mercury would have shown up in a few days of continuous exposure of the gold leaf to the vapor.

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Proc. Nat. Acad. Sciences, 2, p. 683; 1916.

Phys. Rev., 17, p. 7; 1921.

Taken from C. F. Hills curve Fig. 3 for a temperature of 26.3°C; Phys. Rev., 20, p. 265; 1922.

The ion current of .5 divisions with liquid air on the trap is probably due entirely to the steady evolution of gas from the walls of the ionization gauge.

Wright in The American Journal of Scicnce, 13, p. 49; 1877, probably had a large surface of gold compared to the rate of diffusion of the mercury vapor. The chances are, too, that the spectrum of mercury would have shown up in a few days of continuous exposure of the gold leaf to the vapor.

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