The physical realizability and realization of linear phase shift networks
Author:
Paul M. Chirlian
Journal:
Quart. Appl. Math. 18 (1960), 31-35
MSC:
Primary 78.00
DOI:
https://doi.org/10.1090/qam/119805
MathSciNet review:
119805
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Abstract: Necessary and sufficient conditions for the physical realizability of linear phase shift networks are imposed upon the network transfer function. A technique is presented for approximating non-physically realizable transfer functions with those which are physically realizable. It is demonstrated that if the approximation is properly limited, the unit impulse response can be made non-negative for all values of time. These results are extended to networks whose transfer functions phase shift is the sum of two terms, one which varies linearly with frequency and a second which varies in discrete steps of $\pi$ radians.
- Claude E. Shannon, Communication in the presence of noise, Proc. I.R.E. 37 (1949), 10–21. MR 28549
E. C. Titchmarsh, Introduction to the theory of Fourier integrals, Oxford University Press, London, 1948, p. 170
M. S. Corrington and R. W. Sonnenfeldt, Synthesis of constant time delay networks, R. C. A. Rev. 15, 163-186 (June 1954)
H. E. Kallman, Transversal filters, Proc. IRE. 28, 302-310 (July 1940)
C. E. Shannon, Communication in the presence of noise, Proc. IRE 37, 10-21 (Jan. 1949)
E. C. Titchmarsh, Introduction to the theory of Fourier integrals, Oxford University Press, London, 1948, p. 170
M. S. Corrington and R. W. Sonnenfeldt, Synthesis of constant time delay networks, R. C. A. Rev. 15, 163-186 (June 1954)
H. E. Kallman, Transversal filters, Proc. IRE. 28, 302-310 (July 1940)
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Article copyright:
© Copyright 1960
American Mathematical Society