Recovering a finite-energy signal from values of some transforms (Q2761891)
From MaRDI portal
| This is the item page for this Wikibase entity, intended for internal use and editing purposes. Please use this page instead for the normal view: Recovering a finite-energy signal from values of some transforms |
scientific article; zbMATH DE number 1686471
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Recovering a finite-energy signal from values of some transforms |
scientific article; zbMATH DE number 1686471 |
Statements
7 January 2002
0 references
finite energy signal
0 references
wavelets
0 references
integral wavelet transform
0 references
window function
0 references
Recovering a finite-energy signal from values of some transforms (English)
0 references
The author establishes a method to reconstruct any finite energy signal from values of the integral wavelet transform. A function \(f\in L^2(R)\) is used to represent an analog signal with finite energy and one problem is to recover any finite energy signal from values of some transforms. The main result is that for any \(f\in L^2(R)\), NEWLINE\[NEWLINE f(x)=(C_{\psi })^{-1/2}\int_{-\infty }^{+\infty }\int_{-\infty }^{+\infty }[(W_{\psi }f)(b,a)]\psi_{b,a}(x)a^{-2} da db NEWLINE\]NEWLINE at any point \(x\in R\), where \(f\) is a continuous function and \(\psi _{b,a}(t)=|a|^{-1/2}\psi ((t-b)a^{-1})\). Here \(\psi \) is a basic wavelet such that \(\psi \), \(\widehat \psi \) are window functions and \((W_{\psi }f)(b,a)\) is the integral wavelet transform on \(L^2(R)\) (\(a,b\in R\), \(a\neq 0\)).
0 references
0.7642160058021545
0 references
0.7390414476394653
0 references
0.7355347871780396
0 references
0.7316147685050964
0 references