Family of continuous wavelets
Hermitian wavelets are a family of continuous wavelets, used in the continuous wavelet transform. The
Hermitian wavelet is defined as the
derivative of a Gaussian distribution, for each positive
:[1]
![{\displaystyle \Psi _{n}(t)=(2n)^{-{\frac {n}{2}c_{n}\operatorname {He} _{n}\left(t\right)e^{-{\frac {1}{2}t^{2},}](https://wikimedia.org/api/rest_v1/media/math/render/svg/e1fba3aa79bc423ab3006515bbe81c71ba876d5a)
where
![{\displaystyle \operatorname {He} _{n}(x)}](https://wikimedia.org/api/rest_v1/media/math/render/svg/a14cb7440e41048805a63f4c154f4077365f2136)
denotes the
probabilist's Hermite polynomial.
The normalization coefficient
is given by,
![{\displaystyle c_{n}=\left(n^{\frac {1}{2}-n}\Gamma \left(n+{\frac {1}{2}\right)\right)^{-{\frac {1}{2}=\left(n^{\frac {1}{2}-n}{\sqrt {\pi }2^{-n}(2n-1)!!\right)^{-{\frac {1}{2}\quad n\in \mathbb {N} .}](https://wikimedia.org/api/rest_v1/media/math/render/svg/0aa76edec92afa765c551adbb59db047465fc2b3)
The perfector
![{\displaystyle C_{\Psi }](https://wikimedia.org/api/rest_v1/media/math/render/svg/70276f0be6f48a25725d094cc2f8b1b7e229e471)
in the resolution of the identity of the continuous wavelet transform for this wavelet is given by the
formula,
[further explanation needed]![{\displaystyle C_{\Psi }={\frac {4\pi n}{2n-1}](https://wikimedia.org/api/rest_v1/media/math/render/svg/c0627d5b1c6b1bb67227587126190eaa30965adb)
In
computer vision and
image processing, Gaussian derivative operators of different orders are frequently used as a
basis for expressing various types of visual operations; see
scale space and
N-jet.
Examples
The first three derivatives of the Gaussian function with
:
![{\displaystyle f(t)=\pi ^{-1/4}e^{(-t^{2}/2)},}](https://wikimedia.org/api/rest_v1/media/math/render/svg/04c086e7af20ec7dd813ef8ae00a9c1a122a9e97)
are:
![{\displaystyle {\begin{aligned}f'(t)&=-\pi ^{-1/4}te^{(-t^{2}/2)},\\f''(t)&=\pi ^{-1/4}(t^{2}-1)e^{(-t^{2}/2)},\\f^{(3)}(t)&=\pi ^{-1/4}(3t-t^{3})e^{(-t^{2}/2)},\end{aligned}](https://wikimedia.org/api/rest_v1/media/math/render/svg/147c82e75fabd44d0979cf4e3f3388295f1e8850)
and their
![{\displaystyle L^{2}](https://wikimedia.org/api/rest_v1/media/math/render/svg/ba162c66ca85776c83557af5088cc6f8584d1912)
norms
![{\displaystyle ||f'||={\sqrt {2}/2,||f''||={\sqrt {3}/2,||f^{(3)}||={\sqrt {30}/4}](https://wikimedia.org/api/rest_v1/media/math/render/svg/f9dc17cb40345bf6acd3bb5c1fd02843f1527c63)
.
Normalizing the derivatives yields three Hermitian wavelets:
![{\displaystyle {\begin{aligned}\Psi _{1}(t)&={\sqrt {2}\pi ^{-1/4}te^{(-t^{2}/2)},\\\Psi _{2}(t)&={\frac {2}{3}{\sqrt {3}\pi ^{-1/4}(1-t^{2})e^{(-t^{2}/2)},\\\Psi _{3}(t)&={\frac {2}{15}{\sqrt {30}\pi ^{-1/4}(t^{3}-3t)e^{(-t^{2}/2)}.\end{aligned}](https://wikimedia.org/api/rest_v1/media/math/render/svg/b96b833a5049020c00d4221163f8c65ba42a2cfc)
See also
References
External links