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Hilbert transform

Partial Function

definiendum H:(CC)(CC)
definiendum H(f):=y1πPf(x)yxdx

Discussion

(H(f))=f

The Hilbert transform commutes with the Fourier transform up to a simple factor and is an anti-self adjoint operator relative to the duality pairing between Lp(R) and the dual space Lq(R).

It is also used in the Kramers–Kronig relation/Sokhotski–Plemelj theorem to express the imaginary part of an analytic function in terms of its real part (or the other way around). This works because they get “mixed up” in the Cauchy integral formula which introduces a factor of 1i. The principal value is taken to push the complex line integral on the real line.

Reference

Wikipedia: Hilbert transform

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