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I need help finding the Fourier coefficients of:

$f(x) =\begin{cases} \sum_{n=0}^\infty{\frac{e^{inx}}{1+n^2}} & \text{if } x\neq 2k\pi \\0& \text{if } x= 2k\pi \end{cases}$

And my main problem is that I know how to find the coefficients for each case separately, but how do I reach a final answer for the whole function?

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    yes i know that it is already in the form of it's Fourier series for $x\neq 2k\pi$ but, as i originally stated, my problem is how to show that the coefficients are $\frac{1}{1+n^2}$ for the entire function $f$.2012-08-29

2 Answers 2

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According to Mathematica $\sum_{n=0}^\infty{1\over 1+n^2}={1+\pi\,{\rm coth}(\pi)\over2}\doteq 2.07667\ne0\ .$ Therefore your function $f$ differs from the function $g(x):=\sum_{n=0}^\infty {e^{inx}\over 1+n^2}$ only at the points $x=2k\pi$, $\ k\in{\mathbb Z}$. It follows that $f$ has the same Fourier coefficients as $g$, namely $c_n=\cases{{1\over 1+n^2}\quad&$(n\geq0)$ \cr 0&$(n<0)$\cr}\quad .$

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The fourier coefficients of a function depend only on its class in $L^2([0,2\pi])$ so you can think of $f$ to be the series $\sum_{n\geq 0} \dfrac{e^{inx}}{1+n^2}$ since they differ only on the set (of null Lebesgue measure) $2\pi\mathbb Z$.

If you don't really know much about Lebesgue theory, you want to compute the fourier coefficients in terms of the integrals : $c_n(f)=\frac{1}{2\pi}\int_{0}^{2\pi} f(t)e^{-inx}dx$. However you should know that the integral of a function doen't change if you modify its values in a finite number of points.

So the two integrals, with $f$ or with the series, are exactly the same : $c_n(f)=c_n(x\mapsto \sum_{n\geq 0} \frac{e^{inx}}{1+n^2})$.

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    I mean, the function $f$ is clearly $2\pi$-periodic, so information about Fourier coefficients really comes from its restriction to any subset of the form $I_a:=[a,a+2\pi]$. On such a set $f$ differs from $g(x)=\sum_{n\geq 0} \dfrac{e^{inx}}{1+n^2}$ in only two points hence for any continuous function $h:[0,2\pi] \rightarrow \mathbb C$, $\int_0^{2\pi} f(x)h(x)dx= \int_0^{2\pi} g(x)h(x)dx$. It clearly implies that $f$ and $g$ have the same Fourier coefficients and you can see that your question really comes from a construction of the Riemann Integral instead of Fourier formulae.2012-08-29