For , the geometric series gives . Hence this positive even kernel has normalized integral one, and normalized convolution with it multiplies the th Fourier coefficient by . Its mass outside any fixed neighbourhood of zero tends to zero as . If an integrable function has finite one-sided limits at zero, evenness gives half the mass to each side and the convolution tends to .
The Poisson kernel on the circle is nonnegative, has normalized integral one, and its mass outside any fixed arc about zero tends to zero as . Split the convolution error into a short arc, controlled by the modulus of continuity, and its complement, controlled by the vanishing kernel mass. This proves uniform convergence for every continuous periodic function. Its Fourier multiplier is , so the convolution is the Abel sum of the Fourier series.
The geometric series gives . Its convolution multiplier is for nonzero frequencies and zero at frequency zero. Since the series is uniformly absolutely convergent for , these identities hold for every Lebesgue integrable function by termwise integration. If all negative Fourier coefficients vanish, .
Let an integrable function have finite one-sided limits at zero. Oddness gives . Also . Thus : make the near-zero error in arbitrarily small and bound the remaining integral uniformly. When negative Fourier coefficients vanish, the conjugate-kernel identity makes this convolution bounded because tends to . Therefore . A removable discontinuity caused solely by altering a point value is not excluded.
Articles by others on the same topic
There are currently no matching articles.