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Next: Euclidean Distance in Wavelet Up: Introduction to Wavelet Networks Previous: Direct Calculation of Weights

Wavelet basis and Wavelet subspace

Considering the optimized family of wavelets $ {\bf\Psi }$, its closed linear span constitutes a subspace $ <{\bf\Psi}>$ in the $ {\Bbb{L}}^2({\Bbb{R}}^2)$ space. With eq. (8) any function can be orthogonally projected into that subspace. It is interesting to ask whether $ {\bf\Psi }$ constitutes a basis, because then the projection is unique. That this is indeed so can be shown with induction over the number of wavelets: Consider $ n$ wavelets $ (\psi_{{\bf n}_1},\ldots,\psi_{{\bf n}_n})$, that minimize the energy functional (2) and that form a basis. Let us choose a new wavelet that approximates best the residual between the function $ f$ and its approximation with the first $ n$ wavelets. After optimization of the $ n$th$ + 1$ wavelet, the energy functional (2) is smaller than before (for the $ n$ wavelets):

$\displaystyle \Vert f-\sum_{i=1}^n w_i \psi_{{\bf n}_i}\Vert > \Vert f-\sum_{i=1}^n w_i
\psi_{{\bf n}_i} - w_{n+1} \psi_{{\bf n}_{n+1}}\Vert\; .
$

Assuming now, that

$\displaystyle <\psi_{{\bf n}_1},\ldots,\psi_{{\bf n}_n}> =
<\psi_{{\bf n}_1},\ldots,\psi_{{\bf n}_{n+1}}>
$

we have in particular

$\displaystyle <\psi_{{\bf n}_1},\ldots,\psi_{{\bf n}_n}>^{\perp} =
<\psi_{{\bf n}_1},\ldots,\psi_{{\bf n}_{n+1}}>^{\perp}.
$

This again means that

$\displaystyle f-\sum_{i=1}^{n} w_i \psi_{{\bf n}_i} \in
(<\psi_{{\bf n}_1},\ldots,\psi_{{\bf n}_{n+1}}>)^{\perp}\; ,
$

which implies

$\displaystyle \langle
f-\sum_{i=1}^{n} w_i \psi_{{\bf n}_i},\psi_{{\bf n}_{n+1}}
\rangle = 0 \; .
$

This, however, contradicts the choice of $ \psi_{{\bf n}_n}$ in the optimization step, where $ \psi_{{\bf n}_n}$ was selected such that

$\displaystyle \langle
f-\sum_{i=1}^{n} w_i \psi_{{\bf n}_i},\psi_{{\bf n}_{n+1}}
\rangle \neq 0 \; .
$

Let us call the closed linear span of $ <{\bf\Psi}>$ $ {\Bbb{L}}^2({\Bbb{R}}^2)$ (image) subspace. The dual wavelets $ \tilde{\psi}_{{\bf n}_i}$ are linearly independent, and the projection

$\displaystyle {\bf w}= \tilde{{\bf\Psi}}g
$

establishes an isomorphism from $ {\Bbb{L}}^2({\Bbb{R}}^2)$ (or the image space, respectively) into $ \Bbb{R}^n$ which is the space of the $ n$-vectors containing the wavelet coefficients. This space is dual to the image subspace and we call it the wavelet subspace.

Figure: A function $ g \in {\Bbb{L}}^2({\Bbb{R}}^2)$ is mapped by the linear mapping $ \tilde{{\bf \Psi}}$ onto the vector $ {\bf w}\in
\Bbb{R}^N$ in the wavelet subspace. The mapping of $ {\bf w}$ into $ {\Bbb{L}}^2({\Bbb{R}}^2)$ is achieved with the linear mapping $ {\bf \Psi}$. Both mappings constitute an orthogonal projection of a function $ g \in {\Bbb{L}}^2({\Bbb{R}}^2)$ into the (image) subspace $ <{\bf \Psi}> \subset {\Bbb{L}}^2({\Bbb{R}}^2)$.
\begin{center}\vbox{\input{/home/vok/tex/wavelets/fig/mapping.eepic}
}\end{center}


next up previous
Next: Euclidean Distance in Wavelet Up: Introduction to Wavelet Networks Previous: Direct Calculation of Weights
Volker Krueger
2001-05-31