Let , a Schwartz function. Splitting the inverse Fourier transform at the jump in the Hilbert-transform Fourier multiplier gives
For , integration by parts on each half-line shows
Both restricted derivatives are in . The Riemann-Lebesgue lemma makes the bracket tend to zero as . Hence the two-sided tail is
Here . The large-distance tail of the Hilbert transform thus depends on the zeroth moment of the input. If that moment is nonzero, the tail proves that the output is not a Schwartz function, despite being smooth and square-integrable.

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