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Nontrivial Riemann Zeros as Spectrum

Mathematical Physics 2026-03-12 v15 math.MP Quantum Physics

Abstract

Let Λ(s):=Γ(s+1)(121s)ζ(s) \Lambda (s) := \Gamma(s+1)\, (1-2^{1-s}) \, \zeta(s) , and denote its set of zeros by ZΛ:=ZζZp Z_\Lambda := Z_\zeta \cup Z_\mathrm{p} , where Zζ Z_\zeta consists of the nontrivial zeros of ζ(s) \zeta(s) and Zp Z_\mathrm{p} those of the prefactor (121s) ( 1-2^{1-s} ) , with s1 s \neq 1 . We introduce a non-symmetric operator R R on L2([0,)) L^2([0,\infty)) with spectrum σ(R)={i(1/2λ)λZΛ}. \sigma(R) = \left\{ i\left(1/2- \lambda \right) \mid \lambda \in Z_\Lambda \right\} \, . Assuming the simplicity of all nontrivial Riemann zeros, we construct the compression RZζ R_{Z_\zeta} of R R to the spectral subspace associated with Zζ Z_\zeta, and show that RZζ R_{Z_\zeta} is intertwined with its adjoint by a positive semidefinite operator W W ; i.e., WRZζ=RZζW W \, R_{Z_\zeta} = R_{Z_\zeta}^\dagger \, W with W0 W \ge 0 . The positivity of W W , viewed as an operator-theoretic form of (Bombieri's refinement of) Weil's positivity criterion, enforces (ρ)=1/2 \Re(\rho)=1/2 for all ρZζ \rho \in Z_\zeta , in accordance with the Riemann Hypothesis. Under the same positivity condition, the intertwining relation yields a self-adjoint operator whose spectrum coincides with the set {(ρ)ρZζ} \{ \Im(\rho) \mid \rho \in Z_\zeta\} . We further extend the framework to accommodate higher-order nontrivial Riemann zeros, should they exist, and to cover any Mellin-transformable L L -function satisfying a functional equation.

Keywords

Cite

@article{arxiv.2408.15135,
  title  = {Nontrivial Riemann Zeros as Spectrum},
  author = {Enderalp Yakaboylu},
  journal= {arXiv preprint arXiv:2408.15135},
  year   = {2026}
}

Comments

19 pages. This revision extends and clarifies the mathematical derivations. The manuscript has been revised in response to significant comment, ensuring continuous improvement

R2 v1 2026-06-28T18:25:34.094Z