Product Equation for Riemann Zeta Function
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Theorem
There exists a constant $B$ such that:
- $\ds \frac {\map {\zeta'} s} {\map \zeta s} = B - \frac 1 {s - 1} + \frac 1 2 \ln \pi - \frac 1 2 \frac {\map {\Gamma'} {s / 2 + 1} } {\map \Gamma {s / 2 + 1} } + \sum_\rho \paren {\frac 1 {s - \rho} + \frac 1 \rho}$
where:
- $\zeta$ is the Riemann zeta function
- $\rho$ runs over the nontrivial zeros of $\zeta$
- $\Gamma$ is the gamma function.
Proof
Let $\xi$ be the completed Riemann zeta function:
\(\ds \map \xi s\) | \(=\) | \(\ds \frac 1 2 s \paren {s - 1} \pi^{-s / 2} \map \Gamma {\frac s 2} \map \zeta s\) | Definition of Completed Riemann Zeta Function | |||||||||||
\(\ds \) | \(=\) | \(\ds \paren {s - 1} \pi^{-s / 2} \map \Gamma {\frac s 2 + 1} \map \zeta s\) | Gamma Difference Equation: $\map \Gamma {\dfrac s 2 + 1} = \dfrac s 2 \map \Gamma {\dfrac s 2}$ | |||||||||||
\(\ds \leadsto \ \ \) | \(\ds \ln \map \xi s\) | \(=\) | \(\ds \map \ln {s - 1} - \frac s 2 \ln \pi + \ln \map \Gamma {\frac s 2 + 1} + \ln \map \zeta s\) | taking the logarithm of both sides | ||||||||||
\(\text {(1)}: \quad\) | \(\ds \leadsto \ \ \) | \(\ds \quad \ds \frac {\map {\xi'} s} {\map \xi s}\) | \(=\) | \(\ds \frac 1 {s - 1} - \frac 1 2 \ln \pi + \dfrac 1 2 \dfrac {\map {\Gamma'} {s / 2 + 1} } {\map \Gamma {s / 2 + 1} } + \frac {\map {\zeta'} s} {\map \zeta s}\) | taking the derivative of both sides |
We have that the Completed Riemann Zeta Function has Order One.
So, by the Hadamard Factorisation Theorem, there exist constants $A$, $B$ such that:
- $\ds \map \xi s = \map \exp {A + B s} : \prod_\rho \paren {1 - \frac s \rho} \map \exp {\frac s \rho}$
where $\rho$ runs over the zeros of $\xi$, that is, the nontrivial zeros of $\zeta$.
Therefore:
\(\ds \map \xi s\) | \(=\) | \(\ds \map \exp {A + B s} : \prod_\rho \paren {1 - \frac s \rho} \map \exp {\frac s \rho}\) | Hadamard Factorisation Theorem | |||||||||||
\(\ds \leadsto \ \ \) | \(\ds \ln \map \xi s\) | \(=\) | \(\ds A + B s + \sum_\rho \paren {\map \ln {1 - \frac s \rho} + \frac s \rho}\) | taking the logarithm of both sides | ||||||||||
\(\text {(2)}: \quad\) | \(\ds \leadsto \ \ \) | \(\ds \quad \ds \frac {\map {\xi'} s} {\map \xi s}\) | \(=\) | \(\ds B + \sum_\rho \paren {\frac 1 {s - \rho} + \frac 1 \rho}\) | taking the derivative of both sides |
Combining $(1)$ and $(2)$ we have:
\(\ds \frac 1 {s - 1} - \frac 1 2 \ln \pi + \dfrac 1 2 \dfrac {\map {\Gamma'} {s / 2 + 1} } {\map \Gamma {s / 2 + 1} } + \frac {\map {\zeta'} s} {\map \zeta s}\) | \(=\) | \(\ds B + \sum_\rho \paren {\frac 1 {s - \rho} + \frac 1 \rho}\) | ||||||||||||
\(\ds \leadsto \ \ \) | \(\ds \frac {\map {\zeta'} s} {\map \zeta s}\) | \(=\) | \(\ds B + \sum_\rho \paren {\frac 1 {s - \rho} + \frac 1 \rho} - \paren {\frac 1 {s - 1} - \frac 1 2 \ln \pi + \dfrac 1 2 \dfrac {\map {\Gamma'} {s / 2 + 1} } {\map \Gamma {s / 2 + 1} } }\) | |||||||||||
\(\ds \) | \(=\) | \(\ds B - \frac 1 {s - 1} + \frac 1 2 \ln \pi - \frac 1 2 \frac {\map {\Gamma'} {s / 2 + 1} } {\map \Gamma {s / 2 + 1} } + \sum_\rho \paren {\frac 1 {s - \rho} + \frac 1 \rho}\) | rearranging terms |
$\blacksquare$
Warning
The sum $\ds \sum_\rho \frac 1 {\size \rho}$ diverges, so we must be careful of the order in which we take the terms.
By the Functional Equation for Riemann Zeta Function, the zeroes occur in complex conjugate pairs, and:
- $\ds \frac 1 \rho + \frac 1 {\overline \rho} = \frac {2 \map \Re \rho} {\size \rho^2} \le \frac 2 {\size \rho^2}$
and we see by the corollary to Zeroes of Functions of Finite Order that a sum of such terms does converge.