Integral Representations of Riemann auxiliary function

Fuente: arXiv
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Autor principal: de Reyna, Juan Arias
Formato: Preprint
Publicado: 2024
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author de Reyna, Juan Arias
author_facet de Reyna, Juan Arias
contents We prove that the auxiliary function $\mathop{\mathcal R}(s)$ has the integral representation \[\mathop{\mathcal R}(s)=-\frac{2^s π^{s}e^{πi s/4}}{Γ(s)}\int_0^\infty y^{s}\frac{1-e^{-πy^2+πωy}}{1-e^{2πωy}}\,\frac{dy}{y},\qquad ω=e^{πi/4}, \quad\Re s>0,\] valid for $σ>0$. The function in the integrand $\frac{1-e^{-πy^2+πωy}}{1-e^{2πωy}}$ is entire. Therefore, no residue is added when we move the path of integration.
format Preprint
id arxiv_https___arxiv_org_abs_2407_02016
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Integral Representations of Riemann auxiliary function
de Reyna, Juan Arias
Number Theory
Primary 11M06, Secondary 30D99
We prove that the auxiliary function $\mathop{\mathcal R}(s)$ has the integral representation \[\mathop{\mathcal R}(s)=-\frac{2^s π^{s}e^{πi s/4}}{Γ(s)}\int_0^\infty y^{s}\frac{1-e^{-πy^2+πωy}}{1-e^{2πωy}}\,\frac{dy}{y},\qquad ω=e^{πi/4}, \quad\Re s>0,\] valid for $σ>0$. The function in the integrand $\frac{1-e^{-πy^2+πωy}}{1-e^{2πωy}}$ is entire. Therefore, no residue is added when we move the path of integration.
title Integral Representations of Riemann auxiliary function
topic Number Theory
Primary 11M06, Secondary 30D99
url https://arxiv.org/abs/2407.02016