eljose said:
[tex]\chi(1/2-is)=-1[/tex] so the modulus of the function [tex]\chi(1/2-is)[/tex] would be equal to 1.
So? I've already explained that [tex]|\chi(s)|=1[/tex] does not imply s is on the critical line.
eljose said:
so you seem to be very clever to find "gaps" and fails in my works now i have a proof for you that is to proof that the set of functional equation...
[tex]k^{2}\chi(1/2+b-it)=\chi(1/2-b-it)[/tex]
[tex]\chi(1/2-b+it)\chi^{*}(1/2-b+it)=1[/tex]
[tex]k^2=[\chi(1/2-b+it)[/tex] with []=modulus of the complex number
have a fixed b as it solution...and more complicate to prove that the only solutions to it for b and k are k=b+1=1...
I'm not sure I understand what you're saying, but with t=0, k=1, and [tex]b=1/2-\alpha[/tex] where I defined [tex]\alpha[/tex] in
https://www.physicsforums.com/showthread.php?t=84445 we have:
[tex](1)^2\chi(1/2+b)=1=\chi(1/2-b)[/tex]
[tex]\chi(1/2-b)\overline{\chi(1/2-b)}=1[/tex]
and
[tex](1)^2=|\chi(1/2-b)|[/tex]
So this looks like a solution that doesn't have b=0.
Or do you want a k and b that hold for all real values of t? Honestly it's hard to understand what you're saying, your post is really confusing (though bravo for finally using the standard symbol [tex]\chi[/tex]). If this is indeed what you're after your second equation is saying [tex]|\chi(1/2-b+it)|=1[/tex] for all real t, so just use an approximation like
[tex]|\chi(\sigma+it)|\sim\left(\frac{t}{2\pi}\right)^{1/2-\sigma}[/tex]
as [tex]t\rightarrow\infty[/tex], valid in any fixed vertical strip (this follows from Stirlings). This asymptotic implies that the modulus can't always be 1 unless [tex]\sigma=1/2[/tex], i.e. our only possibility is b=0. When b=0 and t is real, [tex]|\chi(1/2+it)|=1[/tex] follows from the definition of [tex]\chi[/tex]. k=-1 or +1 follows from your first or last equation.
eljose said:
i am waiting for your respones oh masterminds of mathematics...
Tell you what, if you'd prefer me to never read or respond to your posts again just ask nicely and you've got it.