Wavelet transform modulus maxima are related to the singularities of the signal.

More precisely, the following theorem proves that
**there cannot be a singularity without a
local maximum of the wavelet transform at the finer
scales.**

This theorem indicates the presence of a maximum at the finer scales where a singularity occurs. In the general case, is sequence of modulus maxima is detected which converges to the singularity. Below are the modulus maxima of the previous example:

A PDF file shows the connection between wavelet modulus maxima and the signal singularities.

Since log

is restricted to log

**Warning:** these are
the modulus maxima of the wavelet transform. Instantanuous
frequencies are detected from the maxima of the *normalized* scalogram:

which differs in two ways: normalization, and the fact that the variable is homogeneous to a frequency, and not to a scale.

When the wavelet is the n^{th} derivative of a gaussian,
the maxima curves are **connected** and go through all of
the finer scales.

The decay rate of the maxima along the curves indicate the order of the isolated singularities (this a consequence of theorems 6.4 et 6.6 when extended to an interval):

The modulus maxima are displayed as a function of the scale in log-log axes, and the slope gives the estimated singularity order. Below is such a curve for two singularities: the solid line corresponds to the singularity at t=14 and the dotted line to the singularity at t=108. Fine scales are on the left.

For t=14, the slope is 1/2, and the signal is 0-Lipschitz here, that is, it has a discontinuity. For t=108, the slope is close to 1, which indicates that the signal is 1/2 Lipschitz here.