Abstract
Equations are derived for the spreading resistance of a flat contact on the surface of a conducting half-space and on an infinite semiconducting film. The values of the factor Q, which depends on the ratio of the contact radius to the layer thickness, are tabulated. Under certain conditions the spreading resistance can be calculated from simple equations.
Similar content being viewed by others
Literature cited
W. Shockley, Electrons and Holes in Semiconductors, van Nostrand, New York (1950), Chapter 4.
R. G. Mazur and D. H. Dickley, J. Electrochem. Soc.,113, No. 3, 255 (1966).
L. B. Valdes, Proc. IRE,42, 420 (1954).
V. L. Kon'kov, Fiz. Tverd. Tela,6, No. 1, 304 (1961).
J. D. Jackson, Classical Electrodynamics, John Wiley, New York (1962).
P. M. Morse and H. Feshbach, Methods of Theoretical Physics, Vol. 2, McGraw-Hill, New York (1953), Chapter 10.
I. S. Gradshtein and I. M. Ryzhik, Tables of Integrals, Sums, Series, and Products [in Russian], FM (1962).
Author information
Authors and Affiliations
Additional information
Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 9, pp. 100–105, September, 1970.
Rights and permissions
About this article
Cite this article
Polyakov, N.N., Kon'kov, V.L. Spreading resistance of a flat circular contact. Soviet Physics Journal 13, 1203–1207 (1970). https://doi.org/10.1007/BF01100554
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF01100554