J. Appl. Phys. 34, 1793 (1963); http://dx.doi.org/10.1063/1.1702682 (11 pages)
Generalized Formula for the Electric Tunnel Effect between Similar Electrodes Separated by a Thin Insulating Film
(Received 3 January 1963)
© 1963 The American Institute of Physics
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- J. C. Fisher and I. Giaever, J. Appl. Phys. 32, 172 (1961)JAPIAU000032000002000172000001. [ISI]
- A. Sommerfeld and H. Bethe, Handbüch der Physik von Geiger und Sched (Julius Springer-Verlag, Berlin, 1933), Vol. 24/2, p. 450.
- R. Holm, J. Appl. Phys. 22, 569 (1951)JAPIAU000022000005000569000001. [ISI]
- R. Holm and B. Kirschstein, Z. Tech. Physik 16, 488 (1935).
- D. Bohm, Quantum Theory (Prentice-Hall, Inc., Englewood Cliffs, New Jersey, 1951), p. 275.
- By the substitution V(x) =
+
(x), we have inherently assumed that the width
s of the barrier in the range Ex>V(x)>
is constant and equal to the barrier width at the Fermi level. This assumption is justified for practical barriers, because
s varies slowly below the Fermi level [Fig. 4 (a)], and the integral has effective values only when Ex
. - Note added in proof. Simmons has shown [see J. G. Simmons, J. Appl. Phys. 34, 238 (1963)JAPIAU000034000001000238000001] that, at relatively low voltages, Eq. (27) reduces to
which is in good quantitative agreement with the experimental results of Knauss and Breslow [ISI]
[see H. P. Knauss and R. A. Breslow, Proc. IRE 50, 1843 (1962)]. - W. R. Smythe, Static and Dynamic Electricity (McGraw-Hill Book Company, Inc., New York, 1950), Chap. IV.
- R. Holm, Electric Contacts Handbook (Springer-Verlag, Berlin, 1958), 3rd ed., p. 433.
- R. Holm and W. Meissner, Z. Physik 74, 715 (1932);, 86, 787 (1933).
- J. G. Simmons, G. J. Unterkofler, and W. W. Allen, Appl. Phys. Letters 2, 78 (1963)APPLAB000002000004000078000001. [ISI]
- A. R. von Hippel, Dielectric Materials and Applications (Tech. Press, Cambridge, Massachusetts, and John Wiley & Sons, Inc., New York, 1961), Pt. V.













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