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SLOW‐ELECTRON BEAM ATTENUATION BY GOLD FILMS
1.S. H. Sze, J. L. Moll, and T. Sugano, Solid‐State Electron. 7, 509 (1964).
2.C. A. Mead, Phys. Rev. Letters 8, 56 (1962).
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5.also, Twenty‐Sixth Annual Conference on Physical Electronics, March 1966.
6.R. W. Soshea and R. C. Lucas, Phys. Rev. 138, A1182 (1965).
7.For evaluation of data at electron energies close to the vacuum level of the gold film, appreciable change of the air‐stabilized gold surface work function upon further deposition of gold in vacuum must be avoided. No change of the exit potential of the film was observed if the vacuum pressure during gold deposition was allowed to rise to near The data were taken under this condition. At pressures during evaporation below a shift in exit potential of 0.6 eV was observed. Since ultraclean gold films have a work function of near 5.3 eV, the air‐stabilized gold surface work function is near 4.7 eV (refs. 8 and 9).
8.J. C. Riviere, Appl. Phys. Letters 7, 172 (1966).
9.R. P. W. Lawson and G. Carter, Appl. Phys. Letters 9, 85 (1966).
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11.A. H. Wilson, Theory of Metals (Cambridge University Press, New York, 1955), p. 264.
12.S. M. Sze, et al., J. Appl. Phys. 37, 2690 (1966).
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