Proving the Dirichlet Conditions using the Dirichlet-Dini Criterion

400 Views Asked by At

I've been reading Oppenheim's "Signals and Systems" (engineering) textbook and it gives the following "Dirichlet conditions" for pointwise convergence of the Fourier series representation of a function $f$ with period $2\pi$:

  1. $f$ is absolutely integrable over its period
  2. $f$ is of bounded variation, i.e. $f$ has a finite number of minima and maxima during a single period
  3. $f$ has a finite number of finite discontinuities during a single period

From another question, the "i.e." part of condition 2 is not true, as there exist functions with bounded variation that have an infinite number of minima or maxima; from the Wikipedia article on Dirichlet Conditions, replacing the above condition 2 with "$f$ has bounded variation" is sufficient.

I've seen the Dirichlet-Dini Criterion on Wikipedia: the Fourier series representation of a $2\pi$-periodic, locally integrable function $f$ converges at $x_0$ to $l$ if: $$ \int_0^\pi \left| \frac{f(x_0 + t) + f(x_0 - t)}{2} - l \right| \frac{dt}{t} < \infty $$

My intuition is that this criterion is a generalization of the above Dirichlet conditions. Is it possible to prove the above Dirichlet conditions (either the finite extrema or bounded variation case) using the Dirichlet-Dini criterion? If so, how would I go about doing this?

1

There are 1 best solutions below

0
On

This is related to the following, where $S_N^f(\theta)$ is the Fourier series truncated to the terms $1,\sin(n\theta),\cos(n\theta)$ for $n=1,2,3,\cdots,N$. $$ S_{N}^f(\theta)-L=\frac{1}{\pi}\int_0^{\pi}D_N(\theta')\left[\frac{f(\theta+\theta')+f(\theta-\theta')}{2}-L\right]d\theta. $$ The Dirichlet-Dini condition is formulated to make sure that the above tends to $0$ as $N\rightarrow 0$, which gives convergence of the Fourier series at $\theta$ to the mean of the left- and right-hand limits of $f$. The Dirichlet kernel is $$ \sum_{n=-N}^{N}e^{in\phi}=\frac{\sin\left[\frac{1}{2}(2N+1)\phi\right]}{\sin\left[\frac{1}{2}\phi\right]} $$