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The Hilbert transform is an L2 isometry and squares to minus the identity
Statement
Assume Countable Choice, use the convention, and let with . The Hilbert transform of The Hilbert transform is the tempered convolution with pv(1/(pi x)) and has signum Fourier multiplier defines, on Schwartz functions, the operator with . Then extends uniquely to a bounded operator on , still denoted , and for every ,
In particular the single point , where vanishes, is a Lebesgue-null set and creates no zero-mode exception. Nonzero constant functions are not in , so there is no constant mode in the domain to transform.
Facts & Assumptions
Given: Countable Choice and the multiplier of the Schwartz Hilbert transform.
For Schwartz the principal-value Hilbert transform satisfies as tempered distributions. The Hilbert transform is the tempered convolution with pv(1/(pi x)) and has signum Fourier multiplier
A measurable multiplier with finite essential supremum defines the bounded operator on ; its Schwartz-core action extends uniquely to , it depends only on the almost-everywhere class of , and . Exact L2 Fourier multiplier norm
Plancherel: is a surjective linear isometry of , so and and . Plancherel theorem
Fourier transformation is injective on tempered distributions. Fourier transform is a topological automorphism of tempered distributions
Proof
The symbol satisfies for every , for every , and the exceptional set is the Lebesgue-null singleton .
For Schwartz , [F2] identifies with an class whose regular tempered distribution has Fourier transform . By [F1], the tempered distribution has the same transform. Injectivity [F4] gives equality of these distributions, so is represented by the class . Thus no membership of the principal value is assumed in this identification.
By [F2] the Schwartz-core action of extends uniquely to a bounded operator on ; by 2.1 the Schwartz action of is that core action, so on , and for , because almost everywhere by 1.1.
Likewise, on the Schwartz core by 1.1 and [F3]; both and are bounded on and agree on the dense Schwartz core, so on all of .
Depends on
Used by
- Hilbert transform does not map L-infinity to L-infinity Counterexample
- Hilbert transform is not strong type (1,1) Counterexample
- Finite sum of Riesz squares in L2 Example
- Hilbert transform of an interval indicator Example
- Hilbert transform of the line Poisson kernel Example
- The Hilbert transform is skew-adjoint on L2 Lemma
- Endpoint map for Hilbert and Riesz transforms Remark
Dependency tree · two levels
38 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)