In his paper about Extremal Functions for the Fourier Transform (see, for example, here? https://projecteuclid.org/download/pdf_1/euclid.bams/1183552525), Jeffrey Vaaler, while trying to build extremal trigonometric polynomials for the function
$$ \psi (x) = \begin{cases} x - \lfloor x \rfloor - 1/2, \; x \ne 0 \\ 0, \; x = 0 \end{cases} $$
states that 'by a classical result of Féjer, the partial sums
$$ S(x,n) = \sum_{l=1}^n \frac{\sin (2\pi l x) }{\pi l } $$
are always positive for $x \in (0,1/2) $.
After some time looking at this assertion, I tried to look for the reference he gives (apparently, a paper by Féjer from the late 1920's on which he shows that), but I could only find that in a Springer website - which means, of course, that it is really expensive to get full access to it, besides it is in German (and my German skills basically inexist).
Another interesting fact is that this assertion holds in the limit. That is, by convergence of Fourier Series - because $\psi$ is fo bounded variation on $(-1/2,1/2)$ - The sequence $S(x,n) \rightarrow \psi (x) $ pointwisely, so, as $\psi(x) > 0$ for $x \in (0,1/2)$, then $ S(x,n) > 0$ for sufficiently large $n = n(x)$.
So, now I'm turning to proving this claim. I've had some ideas:
1 - Trying to differentiate $S(x,n)$ - which gives $ 2 D_n - 2 $, where $D_n$ is the $n-$th Dirichlet kernel - and looking for the behaviour of this derivative in the considered interval. At first, it seemed a little bit difficult to continue this way, but it may be worth to try for some more time.
2 - Writing $S(x,n) = - \psi * D_n $ and studying this defining integral, maybe with some integration by parts or something.
If anyone can ever give me some reference to that and/or give some nice, short proof of this, I would be very thankful. This is not that "essential" for my study, just some kind of interesting fact that I think I should know how to prove.
Here is a one-page proof by Landau: http://www.digizeitschriften.de/dms/img/?PID=GDZPPN002374331 .
Here is a rough translation:
Fejer's conjecture $$ S_{n}\left(x\right)=\sum_{\nu=1}^{n}\frac{\sin\left(\nu x\right)}{\nu}>0\qquad\text{ for }\qquad0<x<\pi $$ was first proved independently by Mr. Jackson and Mr. Gronwall. The following proof is shorter than any known one.
Let $n>1$ and assume that the claim holds for $n-1$. If we suppose $$ 0\overset{!}{=}2\sin\frac{x}{2}\cdot S_{n}'\left(x\right)=2\sin\frac{x}{2}\sum_{\nu=1}^{n}\cos\left(\nu x\right)\overset{\left(\ast\right)}{=}\sin\left[\left(n+\frac{1}{2}\right)x\right]-\sin\frac{x}{2}, $$ then we get for $0<x<\pi$ that $$ \sin\left(nx\right)=\sin\left[\left(n+\frac{1}{2}\right)x\right]\cdot\cos\left(\frac{x}{2}\right)-\cos\left[\left(n+\frac{1}{2}\right)x\right]\cdot\sin\left(\frac{x}{2}\right)\overset{\left(\dagger\right)}{=}\left\{ 0\text{ or }\sin\left(x\right)\right\} \geq0, $$ and hence $$ S_{n}\left(x\right)\geq S_{n-1}\left(x\right)>0. $$ Thus, $S_{n}$ does not have a minimum $\leq0$ in the range $0<x<\pi$ and hence does not assume any values $\leq0$.
Some thoughts added: It seems that at $\left(\ast\right)$ the identity $$ 2\sin\left(x\right)\cos\left(y\right)=\sin\left(x-y\right)+\sin\left(x+y\right), $$ together with a telescoping argument is used to get \begin{eqnarray*} 2\sin\frac{x}{2}\cdot\sum_{\nu=1}^{n}\cos\left(\nu x\right) & = & \sum_{\nu=1}^{n}\sin\left(\left(\frac{1}{2}-\nu\right)x\right)+\sum_{\nu=1}^{n}\sin\left(\left(\nu+\frac{1}{2}\right)x\right)\\ & = & \sum_{\nu=1}^{n}\sin\left(\left(\nu+\frac{1}{2}\right)x\right)-\sum_{\nu=1}^{n}\sin\left(\left(\nu-\frac{1}{2}\right)x\right)\\ & \overset{\ell=\nu-1}{=} & \sum_{\nu=1}^{n}\sin\left(\left(\nu+\frac{1}{2}\right)x\right)-\sum_{\ell=0}^{n-1}\sin\left(\left(\ell+\frac{1}{2}\right)x\right)\\ & = & \sin\left(\left(n+\frac{1}{2}\right)x\right)-\sin\frac{x}{2}. \end{eqnarray*}
At $\left(\dagger\right)$, the following argument seems to be used: Since $\sin\left(\frac{x}{2}\right)=\sin\left[\left(n+\frac{1}{2}\right)x\right]$, the identity $\cos^{2}=1-\sin^{2}$ yields $$ \left(\cos\left[\left(n+\frac{1}{2}\right)x\right]\right)^{2}=\left[\cos\left(\frac{x}{2}\right)\right]^{2}, $$ so that there are two possibilities:
We have $\cos\left[\left(n+\frac{1}{2}\right)x\right]=\cos\left(\frac{x}{2}\right)$. In this case, we get \begin{eqnarray*} & & \sin\left[\left(n+\frac{1}{2}\right)x\right]\cdot\cos\left(\frac{x}{2}\right)-\cos\left[\left(n+\frac{1}{2}\right)x\right]\cdot\sin\left(\frac{x}{2}\right)\\ & = & \sin\left(\frac{x}{2}\right)\cdot\left(\cos\left(\frac{x}{2}\right)-\cos\left[\left(n+\frac{1}{2}\right)x\right]\right)\\ & = & 0. \end{eqnarray*}
We have $\cos\left[\left(n+\frac{1}{2}\right)x\right]=-\cos\left(\frac{x}{2}\right)$. In this case, we get \begin{eqnarray*} & & \sin\left[\left(n+\frac{1}{2}\right)x\right]\cdot\cos\left(\frac{x}{2}\right)-\cos\left[\left(n+\frac{1}{2}\right)x\right]\cdot\sin\left(\frac{x}{2}\right)\\ & = & \sin\left(\frac{x}{2}\right)\cdot\left(\cos\left(\frac{x}{2}\right)+\cos\left(\frac{x}{2}\right)\right)\\ & = & 2\sin\left(\frac{x}{2}\right)\cos\left(\frac{x}{2}\right)\\ & = & \sin\left(x\right). \end{eqnarray*}
This justifies the $\left\{ 0\text{ or }\sin\left(x\right)\right\} $ bracket at $(\dagger)$.