Upper bounds are obtained for the error, termed truncation error, which arises in reconstituting a band-limited function by summing over only a finite number (instead of the requisite infinite number) of samples of this function in an appropriate sampling-theorem expansion. Upper bounds are given for the truncation errors of the Cardinal and Fogel sampling expansions and for "self-truncating" versions of these two sampling expansions; these latter sampling expansions are "self-truncating" in the sense that the upper bounds on their truncation errors are almost always much lower than the upper bounds on the truncation errors of their prototype sampling expansions. All of the upper bounds are given as functions of three parameters: M, the maximum magnitude of the band-limited function; q, the per unit guard band (assuming that the band-limited function is sampled at a rate greater than the Nyquist rate); and N, the measure of the number of samples in the finite summation of terms of the sampling expansion.
[1]
J. W. Tukey,et al.
The Measurement of Power Spectra from the Point of View of Communications Engineering
,
1958
.
[2]
Edmund Taylor Whittaker.
XVIII.—On the Functions which are represented by the Expansions of the Interpolation-Theory
,
1915
.
[3]
Jr. J. Spilker.
Theoretical Bounds on the Performance of Sampled Data Communications Systems
,
1960
.
[4]
Lawrence J. Fogel,et al.
A note on the sampling theorem
,
1955,
IRE Trans. Inf. Theory.
[5]
R. M. Stewart.
Statistical Design and Evaluation of Filters for the Restoration of Sampled Data
,
1956,
Proceedings of the IRE.
[6]
Lawrence J. Fogel,et al.
Some general aspects of the sampling theorem
,
1956,
IRE Trans. Inf. Theory.
[7]
R. Duffin,et al.
Some properties of functions of exponential type
,
1938
.