Math 2.0

Harmonic analysis on Euclidean spaces Wavelets Example

Morlet wavelet

Builds on WaveletContinuous wavelet transformAdmissibility condition for wavelets

Example

Fix a parameter σ>0\sigma > 0 and put κσ=e−σ2/2\kappa_\sigma = e^{-\sigma^2/2}. The Morlet wavelet is the complex-valued function ψσ(t)=cσ π−1/4e−t2/2(eiσt−κσ),t∈ℝ,\psi_\sigma(t) = c_\sigma \, \pi^{-1/4} e^{-t^2/2} \left(e^{i\sigma t} - \kappa_\sigma\right), \qquad t \in \R, where cσ>0c_\sigma > 0 is the constant that makes ∥ψσ∥2=1\norm{\psi_\sigma}_2 = 1. It is a plane wave eiσte^{i\sigma t} under a Gaussian envelope, with a small correction term.

Check of the zero mean. Since ∫ℝe−t2/2eiσt dt=2π e−σ2/2\int_{\R} e^{-t^2/2} e^{i\sigma t} \, dt = \sqrt{2\pi} \, e^{-\sigma^2/2} and ∫ℝe−t2/2 dt=2π\int_{\R} e^{-t^2/2} \, dt = \sqrt{2\pi}, the integral of ψσ\psi_\sigma is cσπ−1/42π(e−σ2/2−κσ)=0c_\sigma \pi^{-1/4} \sqrt{2\pi} \left(e^{-\sigma^2/2} - \kappa_\sigma\right) = 0. Its Fourier transform is a combination of two Gaussians and vanishes at frequency 00. Together with the Gaussian decay, this gives the admissibility condition, so ψσ\psi_\sigma can be used in the continuous wavelet transform.

Remarks

The correction κσ\kappa_\sigma is tiny when σ\sigma is large; for σ≥5\sigma \ge 5 it is below 10−510^{-5}, and in practice it is often dropped. Without the correction, the function e−t2/2eiσte^{-t^2/2} e^{i\sigma t} has nonzero integral, so it is not admissible in the strict sense. The Morlet wavelet does not generate an orthonormal basis; it is used for the continuous transform and for time–frequency analysis of signals. Its real part is even and its imaginary part is odd. Since the wavelet is complex-valued, the modulus of the transform gives an amplitude and the argument gives a phase.

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Further reading

  1. Web https://en.wikipedia.org/wiki/Morlet_wavelet
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IllustratesContinuous wavelet transform, Admissibility condition for wavelets
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