Computing the Riemann Zeta Function Using Fourier Series

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SUMMARY

The discussion focuses on the computation of the Riemann Zeta function using Fourier series, highlighting Euler's identity, which states that ##\zeta(2) = \frac{\pi^2}{6}##. The Riemann Zeta function, defined as ##\zeta(s) = \sum_{j=1}^\infty \dfrac{1}{j^s}## for ##s > 1##, is central to this topic. Participants discuss the derivation of this result and reference related insights on calculating the Zeta function for even values of ##s##. Additionally, there are mentions of broken links to supplementary resources that provide further exploration of the sums of odd powers of ##1/n##.

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zeta.png

Euler’s amazing identity
The mathematician Leonard Euler developed some surprising mathematical formulas involving the number ##\pi##. The most famous equation is ##e^{i \pi} = -1##, which is one of the most important equations in modern mathematics, but unfortunately, it wasn’t invented by Euler.Something that is original with Euler is this amazing identity:
Equation 1: ##1 + 1/4 + 1/9 + 1/16 + … = \pi^2/6##
This is one instance of an important function called the Riemann Zeta function, ##zeta(s)##, which in the case where ##s > 1## is defined by:
Equation 2: ##\zeta(s) = \sum_{j=1}^\infty \dfrac{1}{j^s}##
So Euler’s identity can be written as:
Equation 3: ##\zeta(2) = \frac{\pi^2}{6}##
This post is an attempt to show how you can derive that result, and related...

Continue reading...
 

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Just below the heading "Equation-7". Also same identity below the heading "Equation-9" and before "Sum-1".
##F(x)= \sum_{j=-\infty}^{\infty} e^{ijx}=\sum_{j=-\infty}^{-1} e^{ijx}+1+\sum_{j=0}^{\infty} e^{ijx} ##

Shouldn't it be(?):
##F(x)= \sum_{j=-\infty}^{\infty} e^{ijx}=\sum_{j=-\infty}^{-1} e^{ijx}+1+\sum_{j=1}^{\infty} e^{ijx} ##
 
Paul Colby said:
I've checked chrome and safari and your link is broken in both. There appears to be garbage prior to the working URL. Is this the correct one?
Yes. I have extended the results in that insight and I will update it Really Soon Now (as Jerry Pournelle used to say).
 

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