An integral representation of the Hurwitz zeta function

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Discussion Overview

The discussion centers around the integral representation of the Hurwitz zeta function, exploring its properties, derivations, and connections to other mathematical functions such as the gamma function. The scope includes theoretical aspects and mathematical reasoning related to special functions.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Exploratory

Main Points Raised

  • One participant defines the Hurwitz zeta function and notes its relationship to the Riemann zeta function, mentioning its analytic continuation.
  • Another participant references an article related to the topic, indicating interest in the Negapolygamma functions.
  • A participant suggests that using contour integration simplifies the derivation of the integral representation.
  • One participant presents a derivation that connects the integral representation of the Hurwitz zeta function to a representation of the gamma function, including specific mathematical expressions.
  • Another participant expresses admiration for the previous contributions and shares a link to a paper containing analogous integrals.

Areas of Agreement / Disagreement

Participants express various viewpoints and approaches regarding the integral representation and its implications, but no consensus is reached on the best method or interpretation.

Contextual Notes

The discussion includes complex mathematical expressions and derivations that may depend on specific assumptions or definitions, which are not fully resolved within the thread.

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For $ \text{Re} (a) >0$ and $\text{Re} (s)>1$, the Hurwitz zeta function is defined as $ \displaystyle \zeta(s,a) = \sum_{n=0}^{\infty} \frac{1}{(a+n)^{s}} $.

Notice that $\zeta(s) = \zeta(s,1)$.

So the Hurwitz zeta function is a generalization of the Riemann zeta function.

And just like the Riemann zeta function, the Hurwitz zeta function can be continued analytically to all complex values of $s$ excluding $s=1$.

One way to see this is an integral representation that generalizes the one I recently posted for the Riemann zeta function.

$\displaystyle \zeta(s,a) = 2 \int_{0}^{\infty} \frac{\sin (s \arctan \frac{t}{a} )}{(a^{2}+t^{2})^{s/2} (e^{2 \pi t}-1)} \ dt + \frac{1}{2a^{s}} + \frac{a^{1-s}}{s-1} $

The derivation of this integral representation shouldn't be that much different.

But since this representation is stated almost nowhere, I thought it would be something interesting to post.EDIT: It actually is stated on Wolfram MathWorld.
 
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Using contour integration makes the derivation/proof so much easier.
 
You can derive a simple yet exotic-looking representation of the gamma function from this integral representation of the Hurwitz zeta function.$$ \frac{\partial }{\partial s} \zeta(s,a) \Big|_{s=0} = \zeta'(0,s) = 2 \int_{0}^{\infty} \frac{\arctan (\frac{t}{a})}{e^{2 \pi t}-1} \ dt - \frac{\log a}{2} + a \log a -a $$Binet's integral formula once again states $$ \int_{0}^{\infty} \frac{\arctan \left( \frac{x}{z} \right)}{e^{2 \pi x} -1} \ dx = \ln \Gamma(z) - \left( z- \frac{1}{2} \right) \ln z + z - \frac{\ln (2 \pi)}{2} $$So

$$ \zeta'(0,a) = \log \Gamma(a) - a \log a + \frac{\log a}{2} + a - \frac{\log (2 \pi)}{2} - \frac{\log a}{2} + a \log a -a = \ln \Gamma(a) - \frac{\log (2 \pi)}{2}$$

$$ \implies \Gamma(a) = \sqrt{2 \pi} e^{\zeta'(0,a)} $$(Speechless)

I think my brain just exploded a little bit.
 
Nicely done, RV! (Clapping)

I think I might have recommended this link before, but just in case, the following paper of Adamchik contains quite a few integrals analogous to the one above...

http://arxiv.org/pdf/math/0308086v1.pdf
 

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