Summary
The electrical impedance of a semiconductor supporting two waves contains an entire transcendental function of the form f(z)=exp(−z)−1−cz, wherec is a complex parameter. This function has an infinity of zeros in the left half z-plane when c is finite (0<¦c¦<+∞). Several approximate expressions for the location of zeros as function of c are obtained. For certain values of c (cf. Fig. 3) one or several zeros are located in the right half z-plane. The real part of some of those exceeds an arbitrarily large positive number, provided c is properly chosen. This corresponds to resonances which represent growing oscillations.
Similar content being viewed by others
References
H.Skeie, Collective Wave Propagation and Current Instabilities in a Piezoelectric Semiconductor, Report TE-73, (Electronikklaboratoriet, N.T.H. Trondheim, Norway, 1966), p. 39.
J.Falnes, Unstable resonances in a semiconductor wafer, Internat.J.Electronics, 24, pp. 505–520.
D.E.McCumber and A.G.Chynoweth, Negative Conductance Amplification and Gunn Instabilities in “Two-Valley” Semiconductors, IEEE Trans. Electron Devices, ED13, 4–21 (Jan. 1966).
E.G.Phillips, Functions of a complex variable, 8th ed. p. 108 (Oliver and Boyd, 1957) (First edition 1940).
K.Knopp, Theory of Functions, Part II (Dover, New York, 1947), p. 105, pp. 141–144.
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Falnes, J. Complex zeros of a transcendental impedance function. J Eng Math 2, 389–401 (1968). https://doi.org/10.1007/BF01579580
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF01579580