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Riesz transform : ウィキペディア英語版
Riesz transform
In the mathematical theory of harmonic analysis, the Riesz transforms are a family of generalizations of the Hilbert transform to Euclidean spaces of dimension ''d'' > 1. They are a type of singular integral operator, meaning that they are given by a convolution of one function with another function having a singularity at the origin. Specifically, the Riesz transforms of a complex-valued function ƒ on R''d'' are defined by
\,dt|}}
for ''j'' = 1,2,...,''d''. The constant ''c''''d'' is a dimensional normalization given by
:c_d = \frac{|x|^{d+1}}.
The Riesz transforms arises in the study of differentiability properties of harmonic potentials in potential theory and harmonic analysis. In particular, they arise in the proof of the Calderón-Zygmund inequality .
==Multiplier properties==

The Riesz transforms are given by a Fourier multiplier. Indeed, the ) = \sum_^d \rho_ R_kf.
These three properties in fact characterize the Riesz transform in the following sense. Let ''T''=(''T''''1'',…,''T''''d'') be a ''d''-tuple of bounded linear operators from ''L''2(R''d'') to ''L''2(R''d'') such that
* ''T'' commutes with all dilations and translations.
* ''T'' is equivariant with respect to rotations.
Then, for some constant ''c'', ''T'' = ''cR''.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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