A FULLY INVERTIBLE GLOBAL ANALYTIC MODEL OF THE RIEMANN ZETA FUNCTION

01 September 2025, Version 2
This content is an early or alternative research output and has not been peer-reviewed by Cambridge University Press at the time of posting.

Abstract

We construct a globally invertible analytic model for functions in the Hardy space H2(C+) [6, 17] via an explicit atomic system {Φn}, where each atom is defined to satisfy analyticity, completeness, stability, and modulator regularity [7, 4] by construction. No external hypotheses are required; all structural properties are encoded directly. The family {Φn} forms a Riesz basis of H2(C+) [3], yielding a unique and stable expansion f (s) = ∞ cnΦn(s), f ∈ H2(C+), n=1 which is globally invertible: coefficients can be recovered from analytic data, and synthesis reconstructs the function uniformly on compact subsets [14]. This construction provides a fully explicit, logically self-contained framework for ana- lyzing analytic functions with growth and symmetry constraints, and suggests applications to L-functions and other areas of analytic number theory [15, 1, 5].

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Comment number 3, Sui Mikasa: Sep 01, 2025, 13:21

the third version is ready. You can get this via email. I will send you as possible as quickly

Comment number 2, Sui Mikasa: Sep 01, 2025, 13:10

welcome to any suggestions and thoughts via email:suimikasa@icloud.com

Comment number 1, Sui Mikasa: Sep 01, 2025, 13:09

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.