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From: efji <efji@efi.efji>
Newsgroups: sci.math
Subject: Re: The Reimann "Zeta" function: How can it ever converge?
Date: Tue, 25 Mar 2025 21:57:53 +0100
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Le 25/03/2025 à 20:15, Kenny McCormack a écrit :
> So I was reading in Wikipedia about the Zeta function, which is defined as:
>
> Z(s) = 1/(1**s) + 1/(2**s) + 1/(3**s) + ...
>
> Both the domain and range are specified as the complex numbers.
>
> And it says that if s is a negative integers (-2, -4, -6, etc), then Z(s)
> is zero. But that can't be right. But first, a little manipulation:
>
> Suppose s is -2:
>
> 1/(n**s), where s = -2
>
> is:
>
> 1/(1/(n**2))
>
> is:
>
> n**2
>
> so, the sum is like:
>
> 1+4+9+16+25+...
>
> Which just grows without bounds. And is certainly never zero.
>
> So, is Wikipedia wrong? Or just a typo?
>
I think it is far beyond the scope of this group, but let's try :
The Riemann zeta function (please, Riemann and not Reimann...) is
defined as the following series for any complex s such that Re(s) > 1:
Z(s) = 1/(1**s) + 1/(2**s) + 1/(3**s) + ..
The condition Re(s)>1 ensures the convergence of the series. Elsewhere,
there is an smooth continuation and thus it can be rewritten in the
whole complex plane as
Z(s) = 2^s \pi^{s-1} \sin(\pi s/2) \Gamma(1-s) Z(1-s)
Where \Gamma denotes the gamma-function, i.e. the regular function
defined on the half complex plane Re(z)>0 such that \Gamma(n) = (n-1)!
forall n integer ("n!" denotes "factorial n").
On this expression you can check that Z is then well defined for every
complex number s.
You can also check that if n is an negative even integer, then
Z(n) = 2^n \pi^{n-1} \sin(\pi n/2) \Gamma(1-s) Z(1-n) = 0
since
\sin(\pi n/2) = 0
Be careful, you cannot use the same idea for a positive even integer n,
since Γ has also a smooth continuation of the genuine gamma-function for
Re(z)<0, and this continuation has a pole (i.e. it goes to infinity) for
negative integers. Thus you get a product 0*\infty that has to be
properly treated (and in the end Z(n) is not 0 for n a positive odd
integer).
That's only the "trivial part" of the study of the Riemann zeta function :)
--
F.J.