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I replaced $\zeta^*$ (based on $\zeta$) by $\eta^*$ (based on $\eta$). Further changes will be required, but this is needed first to go in the right direction.

Scaled Riemann zeta function with no zero in the critical strip

Prime numbers are denoted as $p_1,p_2,\dots$ with $p_1=2$. The modulus of a complex number $s$ is denoted as $|s|$. Finally, $S$ denotes the right half of the critical strip, defined by $\frac{1}{2}<\Re(s)<1$.

Let us assume that one can find a product of the form

$$\eta^*(s)=(1-2^{s-1})\prod_{k=1}^\infty\frac{\tau_k(s)}{1-p_k^{-s}},$$

converging in $S$, but not necessarily if $\Re(s)=\frac{1}{2}$, thus leaving open the possibility that it has zeroes or is undefined on the critical line. Let us further assume that if $s\in S$, we have:

  • $\tau_k(s)$ is a strictly positive real number
  • $|\eta^*(s)|>0$, thus no zero (in other words, the product converges if $s\in S$)
  • $\eta^*(s)$ is smooth enough

Would that imply that the Riemann Hypothesis (RH) is true? I guess the answer is not necessarily. I can not believe that the answer is yes, otherwise (barring some mistakes in my computations), I have found such a function, and I know that there is no way I could prove RH. So I am looking for an answer that explains why it does not necessarily imply that RH is true.

Note that if $\tau_k(s)=1$, then $\eta^*=\eta$ is the traditional Dirichlet eta function.

Below is my function $\eta^*$ satisfying all the requirements. The methodology to get there can be applied to other Dirichet $L$-functions. It is described in some details in my previous MO question here (not at all intended to prove RH), with the core idea explained in the "Update" section, just below the conclusions. The arguments are not very complicated. Instead, the approach (based on finite products ultimately converging) is somewhat unusual and involves some subtleties, and some luck in the sense that there are some rather unexpected simplifications taking place.

About my re-scaled Riemann zeta product

Let $s=\sigma + it$. It is defined using

$$\tau_k(s)=\Big[1+\frac{2\cos(t\log p_k)}{p_k^\sigma + p_k^{-\sigma}}\Big]^{-\frac{1}{2}}.$$

It results in

$$|\eta^*(s)|^{-2} = |1-2^{1-s}|^{-2}\Big\{\prod_{k=1}^\infty \Big(1+\frac{1}{p_k^{2\sigma}}\Big)\Big\} \cdot \Big\{\prod_{k=1}^\infty \Big(1-\frac{4\cos^2(t\log p_k)}{p_k^{2\sigma}+p_k^{-2\sigma}+2}\Big)\Big\}.$$

This simplifies to

$$|\eta^*(s)|^{-2} = \frac{|1-2^{s-1}|^{-2}}{\zeta(2\sigma)} \cdot \prod_{k=1}^\infty \Big[1-\Big(\frac{2\cos(t\log p_k)}{p_k^{\sigma}+p_k^{-\sigma}}\Big)^2\Big] .$$

The above product converges if $s\in S$, but not always (if ever) when $\Re(s)=\frac{1}{2}$, and never if $\Re(s)<\frac{1}{2}$. And of course, due to the infinite product representation, $\eta^*(s)$ can never vanish if $s\in S$. Again, details are available here.

Conclusions

Just like $\eta$ (the Dirichlet eta function) is a scaled version of $\zeta$ to study its zeroes in $0<\Re(s)<1$, so is $\eta^*$ in $\frac{1}{2}<\Re(s)<1$. We have $\eta(s)=(1-2^{1-s})\zeta(s)$ and $\eta^*(s)=\tau(s)\eta(s)$ with $\tau(s)$ being the product of all $\tau_k(s)$, properly defined if $\Re(s)>1$. Both functions $\eta$ and $\eta^*$ are scaled analytic continuations of $\zeta$. In particular, $\eta$ is an additive scaling in the sense that it is defined by a series (and thus easy to build but very hard to use to prove RH) while $\eta^*$ is a multiplicative scaling directly defined by an infinite convergent product (thus hard to build but easy to gain insights about RH).