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[parent] value of the Riemann zeta function at $s=2$ (Theorem)

Here we present an application of Parseval's equality to number theory. Let $ \zeta(s)$ denote the Riemann zeta function. We will compute the value

$\displaystyle \zeta(2)$
with the help of Fourier analysis.

Example:

Let $ f\colon \mathbb{R}\to \mathbb{R}$ be the “identity” function, defined by

$\displaystyle f(x)=x,$    for all $\displaystyle x\in\mathbb{R}.$

The Fourier series of this function has been computed in the entry example of Fourier series.

Thus

$\displaystyle f(x)=\ x$ $\displaystyle =$ $\displaystyle a_0^f + \sum_{n=1}^{\infty}(a_n^fcos(nx)+b_n^fsin(nx))$  
  $\displaystyle =$ $\displaystyle \sum_{n=1}^{\infty}(-1)^{n+1}\frac{2}{n} \sin(nx), \quad \forall x\in (-\pi,\pi).$  

Parseval's theorem asserts that:

$\displaystyle \frac{1}{\pi}\int_{-\pi}^{\pi}f^2(x)dx = 2(a_0^f)^2 + \sum_{k=1}^{\infty}[(a_k^f)^2+(b_k^f)^2].$

So we apply this to the function $ f(x)= x $:

$\displaystyle 2(a_0^f)^2 + \sum_{k=1}^{\infty}[(a_k^f)^2+(b_k^f)^2]= \sum_{n=1}^{\infty} \frac{4}{n^2}= 4\sum_{n=1}^{\infty}\frac{1}{n^2}$
and
$\displaystyle \frac{1}{\pi}\int_{-\pi}^{\pi}f^2(x)dx = \frac{1}{\pi}\int_{-\pi}^{\pi}x^2dx= \frac{2\pi^2}{3}.$

Hence by Parseval's equality

$\displaystyle 4\sum_{n=1}^{\infty}\frac{1}{n^2}=\frac{2\pi^2}{3}$
and hence
$\displaystyle \zeta(2)=\sum_{n=1}^{\infty}\frac{1}{n^2}=\frac{\pi^2}{6}.$



"value of the Riemann zeta function at $s=2$" is owned by alozano.
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See Also: example of Fourier series, Parseval equality, values of the Riemann zeta function in terms of Bernoulli numbers


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Cross-references: Parseval's theorem, example of Fourier series, Fourier series, function, Riemann zeta function, number theory, Parseval's equality
There are 3 references to this entry.

This is version 10 of value of the Riemann zeta function at $s=2$, born on 2003-09-10, modified 2004-09-04.
Object id is 4719, canonical name is ValueOfTheRiemannZetaFunctionAtS2.
Accessed 6609 times total.

Classification:
AMS MSC11M99 (Number theory :: Zeta and $L$-functions: analytic theory :: Miscellaneous)
 42A16 (Fourier analysis :: Fourier analysis in one variable :: Fourier coefficients, Fourier series of functions with special properties, special Fourier series)

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Riemann zeta function at $s=0$ by perucho on 2003-09-21 03:20:54
Riemann proved that $\zeta(s)$ is extensible analitically over $\mathbb{C}$ like a meromorphic function having a simple pole with residue $1$ at $s=1$, trivial zeros $\sigma\in2\mathbb{Z}^-$ and non-trivial zeros lying in the critical band.
In a recent work in PM owned by Mr. Alozano, he performed the calculation of $\zeta(2)$ using Fourier series and the well-known Parseval's identity. He got $\zeta(2)=\frac{\pi^2}{6}$, a trascendent irrational number. But not always neither we can evaluate $\zeta(s)$ by using the mentioned technic nor this one is a irrational number. That is the case about $\zeta(0)$. The more expeditive way to catch it was given by Mr. Hammick in its entry: "formulae for zeta in the critical strip". In the semi-plane $\Re(s)>-1$, we have the formula
$$\zeta(s)=\frac{1}{s-1}+\frac{1}{2}-s\int_1^\infty\frac{((x))}{x^{s+1}}dx$$
where $((x))=x-\left\lfloorx\right\rfloor-\frac{1}{2}=<x>-\frac{1}{2}$
Here $<\cdot>$ stands for the fractional function. Next, taking $s=0$,
we get trivially $\zeta(0)=-\frac{1}{2}$, a rational number and, maybe the unique one.
Pedro
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