Difference between revisions of "Functional equation for the zeta function"
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</cmath> | </cmath> | ||
− | in which we can extend the ROC of the latter integral to <math>\sigma>-1</math> via | + | in which we can extend the ROC of the latter integral to <math>\sigma>-1</math> via integration by parts: |
<cmath> | <cmath> | ||
− | \int_1^\infty{B_1(x)\over x^{s+1}}\mathrm dx={B_2(x)\over2x^{s+1}}+{s+1\over2}\int_1^\infty{B_2(x)\over x^{s+2}}\mathrm dx | + | \begin{aligned} |
+ | \int_1^\infty{B_1(x)\over x^{s+1}}\mathrm dx | ||
+ | ={B_2(x)\over2x^{s+1}}+{s+1\over2}\int_1^\infty{B_2(x)\over x^{s+2}}\mathrm dx | ||
+ | \end{aligned} | ||
</cmath> | </cmath> |
Revision as of 02:19, 13 January 2021
Introduction
The functional equation for Riemann zeta function is a result due to analytic continuation of Riemann zeta function:
Proof
Two useful identities
There are multiple proofs for the functional equation for Riemann zeta function, and this page presents a light-weighted approach which merely relies on the Fourier series for the first periodic Bernoulli polynomial that
From to
In this article, we will use the common convention that where . As a result, we say that the original Dirichlet series definition converges only for . However, if we were to apply Euler-Maclaurin summation on this definition, we obtain
in which we can extend the ROC of the latter integral to via integration by parts:
\begin{aligned} \int_1^\infty{B_1(x)\over x^{s+1}}\mathrm dx ={B_2(x)\over2x^{s+1}}+{s+1\over2}\int_1^\infty{B_2(x)\over x^{s+2}}\mathrm dx \end{aligned} (Error compiling LaTeX. Unknown error_msg)