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G - Quantization of a Sinusoidal Input

from APPENDICES

Published online by Cambridge University Press:  06 July 2010

Bernard Widrow
Affiliation:
Stanford University, California
István Kollár
Affiliation:
Budapest University of Technology and Economics
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Summary

The extremely fast rolloff of the characteristic function of Gaussian variables provides nearly perfect fulfillment of the quantization theorems under most circumstances, and allows easy approximation of the errors in Sheppard's corrections by the first terms of their series expression. However, for most other distributions, this is not the case.

As an example, let us study the behavior of the residual error of Sheppard's first correction in the case of a sinusoidal quantizer input of amplitude A.

Plots of the error are shown in Fig. G.1.

It can be observed that neither of the functions is smooth, that is, a high–order Fourier series is necessary for properly representing the residual error in Sheppard's first correction, R1(A, μ) with sufficient accuracy. The maxima and minima of R1(A, μ) obtained for each value of A by changing μ, exhibits oscillatory behavior. For some values of A, for example as A ≈ 1.43q or A ≈ 1.93q (marked by vertical dotted lines in Fig. G.1(b)), the residual error of Sheppard's correction remains quite small for any value of the mean, but the limits of the error jump apart rapidly for values of A even close to these. A conservative upper bound of the error is therefore as high as the peaks in Fig. G.1(b). One could use the envelope of the error function for this purpose.

Type
Chapter
Information
Quantization Noise
Roundoff Error in Digital Computation, Signal Processing, Control, and Communications
, pp. 637 - 662
Publisher: Cambridge University Press
Print publication year: 2008

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