A FULLY INVERTIBLE GLOBAL ANALYTIC MODEL OF THE RIEMANN ZETA FUNCTION
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the third version is ready. You can get this via email. I will send you as possible as quickly
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we have replaced the Gaussian term with an outer function of the form h_n(s) \;=\; \exp\!\left\{\frac{1}{\pi}\int_{-\infty}^{\infty} \frac{\sigma_s}{(t-y)^2+\sigma_s^2}\,\log w_n(t)\,dt • i \frac{1}{\pi}\int_{-\infty}^{\infty} \frac{t-y}{(t-y)^2+\sigma_s^2}\,\log w_n(t)\,dt\right\}. This modification ensures that the construction remains within the Hardy space framework while preserving analyticity and global invertibility. The use of outer functions provides two key advantages: (i) it guarantees independence from any additional zero structure (since outer factors carry no zeros), and (ii) it yields a boundary modulus representation entirely determined by w_n, aligning the model more naturally with canonical Hardy space decompositions.



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