The key property of the o.n. wave packets is that all phase space cell (i.e.,
wave packets) have the same shape
Let us apply the general idea of constructing o.n. wave packets in Section (2.4.1) to obtain o.n. wave packets with Fourier domain windows of variable width. In fact, we shall construct o.n. wave packets with adjacent, but non-overlapping, windows in the Fourier domain, with each window extending exactly over one octave. Thus each positive frequency window is twice as wide as its neighbor on the left.
In the time domain, all o.n. wave packets have
the same half width, namely
. They are
different in that they are related to one another by discrete equal
shifts
in time and also by equal shifts
in frequency. If a signal changes ``slowly'' over time,
i.e., does not change appreciably over a time interval less than the
inter-wave packet spacing
, then the signal
can be represented quite efficiently by a finite wave packet sum. If,
however, the signal changes ``abruptly'', i.e., it changes appreciably
over a time interval small compared to the width, and hence the
spacing, of the wave packets, then the wave packets representation
becomes less efficient. The wave packet sum must contain many high
frequency packets that reinforce each other on one side where the
abrupt change occurs and cancel each other on the other side of that
change.
What is needed is an o.n. set of variable width wave packets. In effect, instead of having a uniform sampling rate, the sampling rate should be variable to accomodate abrupt changes in the signal. Orthonormal wavelets fullfill this requirement.