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332   Chapter Ten


               by a horizontal distance of |B|/T x . This distance must be greater than
               the extent of the transformed (unsampled) function in x. Similar re-
               sults can be found for all other replicas, but this defines the lower
               bound on the sampling rate.

                                             |B|
                                         T x ≤                     (10.32)
                                              w
               When this bound is used in addition to the Nyquist criterion, the PSD
               of the output waveform—after this is also sampled at the generalized
               Nyquist rate—will look like Fig. 10.10b. Equation (10.32) fails for B=0,
               which is a special case of the LCT where the output is already discrete
               and no second sampling process takes place.




          10.6 Conclusion
               In conclusion we have demonstrated the usefulness of the WDF in
               both qualitatively and quantitatively understanding sampling theory.
               In particular, the ability of the WDF to describe generalized sampling
               is extraordinary. At no point is it necessary to employ a wave integral
               in these derivations. In fact, almost all the equations in this chapter
               serve as a pretext to the underlying idea; by visualizing a signal’s
               energy as a bounded shape in phase space and endowing this shape
               with the basic properties of the WDF, we may derive complicated
               sampling criteria and interpolation formula.



          References
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