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These labels describe origin, not correctness: citations and verification chips remain separate evidence.
Riesz transforms are L2 contractions and square to minus the identity in sum
Statement
Assume Countable Choice and let . For the Riesz transforms of the multiplier definition,
and
Both statements are statements only; no bound for is asserted, and the operators are the operators of the definition, so all identities hold as classes (no pointwise statement is made).
Facts & Assumptions
Given: Countable Choice, the dimension , and the Riesz transforms with symbols for and .
Each is defined as the bounded operator with multiplier ; the symbol is measurable with everywhere, the value at the origin is immaterial, and the definition asserts no more than the multiplier description. Riesz transforms on Euclidean space
A measurable multiplier with finite essential supremum defines the bounded operator with , and depends only on the almost-everywhere class of . Exact L2 Fourier multiplier norm
Plancherel: is a surjective complex-linear isometry of , so . Its inverse is complex-linear, hence and for every class . Plancherel theorem
Proof
For every the symbol values satisfy , while ; the single point is Lebesgue null. Hence the function is measurable, bounded with , and equals the constant almost everywhere.
By [F2] applied to the bounded measurable symbol of [F1], ; consequently, for and using the isometry of [F3], .
Since , composition gives in the notation of [F2], and summing the finitely many bounded operators gives for the almost-everywhere- symbol of 1.1.
By [F2] the operator depends only on the almost-everywhere class of , which by 1.1 is the class of the constant ; hence , and by the linearity and isometry of [F3]. Therefore for every .
Depends on
Used by
Dependency tree · two levels
27 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- Loukas Grafakos, Classical Fourier Analysis, third edition (standard reference, not scraped)
- Richard S. Laugesen, Harmonic Analysis Lecture Notes (standard reference, not scraped)