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Distinction between Contact-Potential Effects and True Reflection Coefficients for Low-Velocity Electrons

H. E. Farnsworth and V. H. Goerke

  • Brown University, Providence, R. I.

Phys. Rev. 36, 1190 – Published 1 October, 1930

DOI: https://doi.org/10.1103/PhysRev.36.1190

Abstract

A method is described for determining the apparent electron reflection coefficient in two ways in the same apparatus such that a distinction may be made between a contact potential and a true reflection coefficient for very low-velocity electrons. The results indicate that for a copper target which has been heated at red heat for some time in a high vacuum, the true electron reflection coefficient approaches a zero value as the primary voltage approaches zero, and that the apparent increase in the reflection coefficient below about one volt, is due to a change in the contact potential between the target and the surrounding electrodes. The value of this change for the specimen tested is approximately 1.2 volts.

References (4)

  1. H. E. Farnsworth, Phys. Rev. 20, 358 (1922)
  2. L. Nordheim, Zeits. f. Physik 46, 833 (1928) Proc. Roy. Soc. A121, 626 (1928)
  3. H. E. Farnsworth, Phys. Rev. 34, 679 (1929)
  4. H. E. Farnsworth, J.O.S.A. & R.S.I. 15, 290 (1927)

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