Complex Mexican hat wavelet

In applied mathematics, the complex Mexican hat wavelet is a low-oscillation, complex-valued, wavelet for the continuous wavelet transform. This wavelet is formulated in terms of its Fourier transform as the Hilbert analytic signal of the conventional Mexican hat wavelet:

Ψ ^ ( ω ) = { 2 2 3 π 1 4 ω 2 e 1 2 ω 2 ω 0 0 ω 0. {\displaystyle {\hat {\Psi }}(\omega )={\begin{cases}2{\sqrt {\frac {2}{3}}}\pi ^{-{\frac {1}{4}}}\omega ^{2}e^{-{\frac {1}{2}}\omega ^{2}}&\omega \geq 0\\0&\omega \leq 0.\end{cases}}}

Temporally, this wavelet can be expressed in terms of the error function, as:

Ψ ( t ) = 2 3 π 1 4 ( π ( 1 t 2 ) e 1 2 t 2 ( 2 i t + π erf [ i 2 t ] ( 1 t 2 ) e 1 2 t 2 ) ) . {\displaystyle \Psi (t)={\frac {2}{\sqrt {3}}}\pi ^{-{\frac {1}{4}}}\left({\sqrt {\pi }}\left(1-t^{2}\right)e^{-{\frac {1}{2}}t^{2}}-\left({\sqrt {2}}it+{\sqrt {\pi }}\operatorname {erf} \left[{\frac {i}{\sqrt {2}}}t\right]\left(1-t^{2}\right)e^{-{\frac {1}{2}}t^{2}}\right)\right).}

This wavelet has O ( | t | 3 ) {\displaystyle O\left(|t|^{-3}\right)} asymptotic temporal decay in | Ψ ( t ) | {\displaystyle |\Psi (t)|} , dominated by the discontinuity of the second derivative of Ψ ^ ( ω ) {\displaystyle {\hat {\Psi }}(\omega )} at ω = 0 {\displaystyle \omega =0} .

This wavelet was proposed in 2002 by Addison et al.[1] for applications requiring high temporal precision time-frequency analysis.

References

  1. ^ P. S. Addison, et al., The Journal of Sound and Vibration, 2002 Archived 2000-02-26 at archive.today