Oddity of a functional equation for the R zeta function

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SUMMARY

The discussion centers on the functional equation of the Riemann zeta function, specifically ζ(s) = ζ(1-s), which indicates symmetry around Re(s) = 1/2. This symmetry contradicts the claim that the Riemann zeta function lacks symmetry along any vertical line. The completed zeta function, denoted as Λ(s), is defined as Λ(s) = (1/2)π^(-s/2)s(s-1)Γ(s/2)ζ(s) and satisfies the equation Λ(s) = Λ(1-s). The conversation also touches on the implications of the Gamma function in establishing this symmetry and the visual representation of transformations in the zeta function.

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nomadreid
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TL;DR
ζ(s)=ζ(1-s) for the zeta function seems to indicate a symmetry around Re(s)=1/2, but this is odd....
In https://empslocal.ex.ac.uk/people/staff/mrwatkin/zeta/fnleqn.htm the equation

ζ(s)=ζ(1-s) is used, where ζ is the Riemann zeta function, which I find curious, for the following reasons

this indicates a symmetry around Re(s)=1/2, which seems to be what the diagram at 20:27 of seems to imply, but contradicting the statement " The Riemann zeta function is not symmetric along with any vertical line at all " from https://www.quora.com/Is-the-Riemann-zeta-function-symmetrical

as well as the elementary consideration that on the real axis there are the trivial zeros in the negative reals that have no corresponding zeros in the positive-real-part side.

(Note that I am not asking about the symmetry ζ(s)=ζ(s*), which is more reasonable.)

What am I missing? Thanks in advance for your patience; I presume this question has been asked many times before (although I couldn't find a good answer with my Internet search).
 
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The functional equations is not for the zeta itself, but for the completed one.

##\zeta(s) = \sum_{n=1}^\infty \frac1{n^s}##

##\Lambda(s) = \frac12 \pi^{\frac{-s}2}s(s-1)\Gamma(\frac s2) \zeta(s)##

then

##\Lambda(s) = \Lambda(1-s)##
 
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Ah, super! Many thanks to both answers! martinbn's answer makes complete sense and clears my question about the equation up; fresh_42's links will provide valuable resources.

A side question, if I may: the 3Blue1Brown video (reference above) seems to be indicating a more complicated symmetry between the part for Re(s)>1 and Re(s)<1 -- his explanation is rather hand-wavy on that. That is, transforming the grid lines on each half of Re(s)=1, he graphs:

bluebrown3.png

(How he graphs this is explained nicely in aheight's answer (post#2) in https://www.physicsforums.com/threads/video-analytic-continuation-seems-to-mix-4-d-2-d-maps.944596/ )

Although my question is rather broad, any hints that anyone could give about this symmetry would be highly appreciated. Either a quick equation as in martinbn's reply, or an indication as to where in the links provided by fresh_42 I might find the answer. Thanks again!
 
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The symmetry is given by ##\xi(s)=\xi(1-s)## where ##\xi(s)=\underbrace{\pi^{-s/2}\,\Gamma(s/2)}_{=c_s} \zeta(s).##

To get from the asymmetric ##\zeta(s)## to the symmetric ##\xi(s)## we need a correction factor ##c_s## which depends on the Gamma-function. And Euler has proven
$$\Gamma(z)\Gamma(1-z) = \dfrac{\pi}{\sin \pi z}\;\text{ for all }z\in \mathbb{C}-\mathbb{Z}$$
I suppose that "bending the grid lines" is a result of visualizing this property of the Gamma-function but I can only guess what exactly they did there. Maybe https://www.wolframalpha.com/input?i=y=pi/(Gamma(ix)*sin(pi+*+i*+x)) is an indication.
 
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fresh_42 said:
The symmetry is given by ##\xi(s)=\xi(1-s)## where ##\xi(s)=\underbrace{\pi^{-s/2}\,\Gamma(s/2)}_{=c_s} \zeta(s).##

To get from the asyymetric ##\zeta(s)## to the symmetric ##\xi(s)## we need a correction factor ##c_s## which depends on the Gamma-function. And Euler has proven
$$\Gamma(z)\Gamma(1-z) = \dfrac{\pi}{\sin \pi z}\;\text{ for all }z\in \mathbb{C}-\mathbb{Z}$$
I suppose that "bending the grid lines" is a result of visualizing this property of the Gamma-function but I can only guess what exactly they did there. Maybe https://www.wolframalpha.com/input?i=y=pi/(Gamma(ix)*sin(pi+*+i*+x)) is an indication.
In the video he gives an example what he means by "bending the grid lines" by using the simpler transformation f(z)=z2: so he takes for example the grid line z: Im(z)=2i, so that if you square each point r+2i in the grid line (r real), you get (r+2i)2=(r2-4)+4ri, so that the line
{z| ∃r∈ℝ: z=(r2-4)+4ri is "bent" (and rotated) compared to the original line.
Roughly,blue to green:
bent.png

So, it appears that the graph referred to in the last post would be looking at the zeta function as a transformation (or, a pair of transformations, one on either side of Re(s)=1) composed of rotations and scaling, so that between each z and ζ(z), a path is traced.
 
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