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Integral Representations of Riemann auxiliary function

Number Theory 2024-07-03 v1

Abstract

We prove that the auxiliary function R(s)\mathop{\mathcal R}(s) has the integral representation R(s)=2sπseπis/4Γ(s)0ys1eπy2+πωy1e2πωydyy,ω=eπi/4,s>0,\mathop{\mathcal R}(s)=-\frac{2^s \pi^{s}e^{\pi i s/4}}{\Gamma(s)}\int_0^\infty y^{s}\frac{1-e^{-\pi y^2+\pi \omega y}}{1-e^{2\pi \omega y}}\,\frac{dy}{y},\qquad \omega=e^{\pi i/4}, \quad\Re s>0, valid for σ>0\sigma>0. The function in the integrand 1eπy2+πωy1e2πωy\frac{1-e^{-\pi y^2+\pi \omega y}}{1-e^{2\pi \omega y}} is entire. Therefore, no residue is added when we move the path of integration.

Cite

@article{arxiv.2407.02016,
  title  = {Integral Representations of Riemann auxiliary function},
  author = {Juan Arias de Reyna},
  journal= {arXiv preprint arXiv:2407.02016},
  year   = {2024}
}

Comments

10 pages 1 figure

R2 v1 2026-06-28T17:26:05.799Z