Deprecated: $wgMWOAuthSharedUserIDs=false is deprecated, set $wgMWOAuthSharedUserIDs=true, $wgMWOAuthSharedUserSource='local' instead [Called from MediaWiki\HookContainer\HookContainer::run in /var/www/html/w/includes/HookContainer/HookContainer.php at line 135] in /var/www/html/w/includes/Debug/MWDebug.php on line 372
Wavelet bases for confinements of the infrared divergence - MaRDI portal

Wavelet bases for confinements of the infrared divergence (Q1021406)

From MaRDI portal





scientific article; zbMATH DE number 5562678
Language Label Description Also known as
English
Wavelet bases for confinements of the infrared divergence
scientific article; zbMATH DE number 5562678

    Statements

    Wavelet bases for confinements of the infrared divergence (English)
    0 references
    0 references
    8 June 2009
    0 references
    The construction of wavelet bases with pseudo-polynomials adapted to the homogeneous Sobolev spaces \(\dot{H}^{s}(\mathbb{R}^{n}), s - n/2\in \mathbb N\) is proposed. This basis is constructed from a Daubechies wavelet basis. A confinement of the infrared divergence via an adapted wavelet analysis is obtained. It means that \(\dot{H}^{s}(\mathbb{R}^{n})\) is decomposed as a direct sum \(X \oplus Y\) where \(X\) is a ``small'' space which carries the divergence and \(Y\) can be embedded in \(\mathcal {S}'(\mathbb{R}^{n})\). An orthonormal basis is constructed in the case of \(\dot{H}^{1}(\mathbb{R}^{2})\). This basis provides an optimal confinement of the Mumford process. It is not a wavelet basis. The possibility to obtain an orthonormal wavelet basis made of compactly supported functions is discussed.
    0 references
    homogeneous Sobolev spaces
    0 references
    wavelet bases
    0 references
    infrared divergence
    0 references
    Mumford process
    0 references
    compactly supported functions
    0 references

    Identifiers