English

Riemann's zeta function and the broadband structure of pure harmonics

General Mathematics 2016-03-14 v1

Abstract

Let a(0,1)a\in (0,1) and let Fs(a)F_s(a) be the periodized zeta function that is defined as Fs(a)=nsexp(2πina)F_s(a) = \sum n^{-s} \exp (2\pi i na) for s>1\Re s >1, and extended to the complex plane via analytic continuation. Let sn=σn+itn,tn>0s_n = \sigma_n + it_n, \, t_n >0 , denote the sequence of nontrivial zeros of the Riemann zeta function in the upper halfplane ordered according to nondecreasing ordinates. We demonstrate that, assuming the Riemann Hypothesis, the Ces\`{a}ro means of the sequence Fsn(a)F_{s_n} (a) converge to the first harmonic exp(2πia)\exp (2\pi i a) in the sense of periodic distributions. This reveals a natural broadband structure of the pure tone. The proof involves Fujii's refinement of the classical Landau theorem related to the uniform distribution modulo one of the nontrivial zeros of ζ\zeta.

Keywords

Cite

@article{arxiv.1603.03667,
  title  = {Riemann's zeta function and the broadband structure of pure harmonics},
  author = {Artur Sowa},
  journal= {arXiv preprint arXiv:1603.03667},
  year   = {2016}
}

Comments

9pages, 1 figure