Searcharxiv⌕ Search

arXiv subjects

Juan Arias de Reyna

Publications and source records attributed to Juan Arias de Reyna.

At least 19 recordsLinked to original sources

Integer complexity: Stability and self-similarity

Define $||n||$ to be the complexity of $n$, the smallest number of ones needed to write $n$ using an arbitrary combination of addition and multiplication. The set $\mathscr{D}$ of defects, differences $δ(n):=||n||-3\log_3 n$, is known to be a well-ordered subset of $[0,\infty)$, with order type $ω^ω$. This is proved by showing that, for any $r$, there is a finite set $\mathcal{S}_s$ of certain multilinear polynomials, called low-defect polynomials, such that $δ(n)\le s$ if and only if one can write $n = f(3^{k_1},\ldots,3^{k_r})3^{k_{r+1}}$. In this paper we show that, in addition to it being true that $\mathscr{D}$ (and thus $\overline{\mathscr{D}}$) has order type $ω^ω$, this set satisifies a sort of self-similarity property with $\overline{\mathscr{D}}' = \overline{\mathscr{D}} + 1$. This is proven by restricting attention to substantial low-defect polynomials, ones that can be themselves written efficiently in a certain sense, and showing that in a certain sense the values of these polynomials at powers of $3$ have complexity equal to the naïve upper bound most of the time. As a result, we also prove that, under appropriate conditions on $a$ and $b$, numbers of the form $b(a3^k+1)3^\ell$ will, for all sufficiently large $k$, have complexity equal to the naïve upper bound. These results resolve various earlier conjectures of the second author.

math.NT↗

Asymptotic properties of zeros of Riemann zeta function

We try to define the sequence of zeros of the Riemann zeta function by an intrinsic property. Let $(z_k)_{k\in \mathbb{N}}$ be the sequence of nontrivial zeros of $ζ(s)$ with positive imaginary part. We write $z_k= 1/2+iτ_k$ (RH says that these $τ_k$ are all real). Then the sequence $(τ_k)_{k\in \mathbb{N}},$ satisfies the following asymptotic relation \[\sum_{k\in\mathbb{N}}\frac{2x}{x^2+τ_k^2}\simeq \frac12\log\frac{x}{2π}+\sum_{n=1}^\infty \frac{a_n}{x^n},\,\,x\to +\infty\] where $a_{2n+1}=2^{-2n-2}(8-E_{2n})$, $a_{2n}=(1-2^{-2n+1})B_{2n}/(4n).$ Are there other sequences $(α_k)_{k\in \mathbb{N}},$ of real or complex numbers enjoying this property? These problems are addressed in this note.

math.NT↗

On convergence of points to limiting processes, with an application to zeta zeros

This paper considers sequences of points on the real line which have been randomly translated, and provides conditions under which various notions of convergence to a limiting point process are equivalent. In particular we consider convergence in correlation, convergence in distribution, and convergence of spacings between points. We also prove a simple Tauberian theorem regarding rescaled correlations. The results are applied to zeros of the Riemann zeta-function to show that several ways to state the GUE Hypothesis are equivalent. The proof relies on a moment bound of A. Fujii.

math.NT↗

Simple bounds for the auxiliary function of Riemann

We give simple numerical bounds for $ζ(s)$, $\vartheta(s)$, $\mathop{\mathcal R}(s)$, $Z(t)$, for use in the numerical computation of these functions. The purpose of the paper is to give bounds for several functions needed in the calculation of $ζ(s)$ and $Z(t)$. We are not pretending to have any originality. Our object is to be useful as a reference in our work for simple (simple to compute and simple to check) bounds.

math.NT↗

A naive integral

In arXiv:2406.0243 two real functions $g(x,t)$ and $f(x,t)$ are defined, so that the Riemann-Siegel $Z$ function is given as \[Z(t)=\mathop{\mathrm{Re}}\Bigl\{\frac{u(t)e^{\frac{πi}{8}}}{\frac12+it}\int_0^\infty g(x,t)e^{i f(x,t)}\,dt\Bigr\},\] where $u(t)$ is a real function of order $t^{-1/4}$ when $t\to+\infty$. The function $g(x,t)$ is indefinitely differentiable and tends to $0$ as well as all its derivatives when $x\to0^+$ or $x\to+\infty$. Since, furthermore, for $t\to+\infty$ the function $f(x,t)$ tends to $+\infty$ we may expect that the integral depends essentially on the behavior of $g(x,t)$ at the extremes. As Polya in an analogous situation we consider the substitution of $ψ(x)$ by a simpler similar function. A simple function with this behavior is \[ψ_0(x):=2π(1+\tfrac{1}{4}x^{-5/2})e^{-πx-\fracπ{4x}}.\] Therefore, we define $J_0(t)$ replacing in the definition of $J(t)$ the function $ψ(x)$ by the simpler $ψ_0(x)$. \begin{equation} J_0(t)=2π\int_0^\infty (1+\tfrac{1}{4}x^{-\frac52})e^{-πx-\fracπ{4x}}(1-ix)^{\frac12(\frac12+it)}\,dx. \end{equation} The resulting $Z_0(t)$ disappoints us \[Z_0(t)\asymp \mathop{\mathrm{Re}}\Bigl\{\frac{2}{\sqrtπ}\exp\Bigl\{i\Bigl(\frac{t}{2}\log\frac{t}{2π}-\frac{t}{2}-\fracπ{8}\Bigr)\Bigr\}+\frac{2}{(2πt)^{1/4}}\exp\Bigl(πi\sqrt{\frac{t}{2π}}\;\Bigr)\Bigr\},\quad t\to+\infty.\] However, the integral $J_0(t)$ is interesting as a technical challenge. And still we have the possibility to get a better result improving $ψ_0(x)$. This is a preliminary version, and we set it as a challenge: to compute and study this integral.

math.NT↗

Levinson Functions

Starting from some of Norman Levinson's results, we construct interesting examples of functions $f(s)$ such that for $s=\frac12+it$, we have $Z(t)=2\Re\{π^{-\frac{s}{2}}Γ(s/2)f(s)\}$. For example one such function is \[\begin{aligned}{\mathcal R }_{-3}(s)=\frac12&\int_{0\swarrow1}\frac{x^{-s}e^{3πix^2}}{e^{πi x}-e^{-πi x}}\,dx\\&+\frac{1}{2\sqrt{3}}\int_{0\swarrow1}\frac{x^{-s}e^{\frac{πi}{3}x^2}}{e^{πi x}-e^{-πi x}}\Bigl(e^{\frac{πi}{2}}+2e^{-\frac{πi}{6}}\cos(\tfrac{2πx}{3})\Bigr)\,dx.\end{aligned}\]

math.NT↗

Integral Representations of Riemann auxiliary function

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.

math.NT↗

Explicit van der Corput's $d$-th derivative estimate

We give an explicit version for van der Corput's $d$-th derivative estimate of exponential sums. $ \textbf{Theorem.}$ Let $X$, and $Y\in\mathbb{R}$ be such that $\lfloor Y\rfloor>d$ where $d\ge3$ is a natural number. Let $f\colon(X,X+Y]\to\mathbb{R}$ be a real function with continuous derivatives up to the order $d$. Assume that $0<λ\le f^{(d)}(x)\leΛ$ for $X<x\le X+Y$. Denote by $D=2^d$. Then \begin{equation}\Bigl|\frac{1}{Y}\sum_{X<n\le X+Y}e(f(n))\Bigr|\le\max\Bigl\{A_d\Bigl(\fracΛ{λY}\Bigr)^{2/D}, B_d\Bigl(\frac{Λ^2}λ\Bigr)^{1/(D-2)},C_d(λY^d)^{-2/D}\Bigr\},\end{equation} where $A_d$, $B_d$, and $C_d$ are explicit constants. They depend on $d$ but for $d\ge2$ for example $A_d< 7.5$, $B_d<5.8$ and $C_d<10.9$. We follow the reasoning of van der Corput in three papers published in 1937, that contained an error. I correct this error and try to get the smallest possible constants. We apply this theorem to zeta sums, giving the best choice of $d$ in each case. Also, we prove that our Theorem implies Titchmarsh's Theorem 5.13.

math.NT↗

An Integral representation of $\mathop{\mathcal R}(s)$ due to Gabcke

Gabcke proved a new integral expression for the auxiliary Riemann function \[\mathop{\mathcal R}(s)=2^{s/2}π^{s/2}e^{πi(s-1)/4}\int_{-\frac12\searrow\frac12} \frac{e^{-πi u^2/2+πi u}}{2i\cosπu}U(s-\tfrac12,\sqrt{2π}e^{πi/4}u)\,du,\] where $U(ν,z)$ is the usual parabolic cylinder function. We give a new, shorter proof, which avoids the use of the Mordell integral. And we write it in the form \begin{equation}\mathop{\mathcal R}(s)=-2^s π^{s/2}e^{πi s/4}\int_{-\infty}^\infty \frac{e^{-πx^2}H_{-s}(x\sqrtπ)}{1+e^{-2πωx}}\,dx.\end{equation} where $H_ν(z)$ is the generalized Hermite polynomial.

math.NT↗

An entire function defined by Riemann

In one of the sheets in Riemann's Nachlass he defines an entire function and connect it with his zeta function. As in many pages in his Nachlass, Riemann is not giving complete proofs. However, I consider that this work is undoubtedly by Riemann. He obtains an $L^\infty$ function whose Fourier transform vanish at the real values $γ$ with $ζ(\frac12+iγ)=0$. We give proofs of Riemann formulas. This is an integral representation of the zeta function different from the known ones. I believe this is the first time it has been published.

math.NT↗

Integral Representation for Riemann-Siegel $Z(t)$ function

We apply Poisson formula for a strip to give a representation of $Z(t)$ by means of an integral. \[F(t)=\int_{-\infty}^\infty \frac{h(x)ζ(4+ix)}{7\coshπ\frac{x-t}{7}}\,dx, \qquad Z(t)=\frac{\Re F(t)}{(\frac14+t^2)^{\frac12}(\frac{25}{4}+t^2)^{\frac12}}.\] After that we get the estimate \[Z(t)=\Bigl(\frac{t}{2π}\Bigr)^{\frac74}\Re\bigl\{e^{i\vartheta(t)}H(t)\bigr\}+O(t^{-3/4}),\] with \[H(t)=\int_{-\infty}^\infty\Bigl(\frac{t}{2π}\Bigr)^{ix/2}\frac{ζ(4+it+ix)}{7\cosh(πx/7)}\,dx=\Bigl(\frac{t}{2π}\Bigr)^{-\frac74}\sum_{n=1}^\infty \frac{1}{n^{\frac12+it}}\frac{2}{1+(\frac{t}{2πn^2})^{-7/2}}.\] We explain how the study of this function can lead to information about the zeros of the zeta function on the critical line.

math.NT↗

Approximate formula for $Z(t)$

The series for the zeta function does not converge on the critical line but the function \[G(t)=\sum_{n=1}^\infty \frac{1}{n^{\frac12+it}}\frac{t}{2πn^2+t}\] satisfies $Z(t)=2\Re\{e^{i\vartheta(t)}G(t)\}+O(t^{-\frac56+\varepsilon})$. So one expects that the zeros of zeta on the critical line are very near the zeros of $\Re\{e^{i\vartheta(t)}G(t)\}$. There is a related function $U(t)$ that satisfies the equality $Z(t)=2\Re\{e^{i\vartheta(t)}U(t)\}$.

math.NT↗

An expression for Riemann Siegel function

There are many analytic functions $U(t)$ satisfying $Z(t)=2\Re\bigl\{ e^{i\vartheta(t)}U(t)\bigr\}$. Here, we consider an entire function $\mathop{\mathcal L}(s)$ such that $U(t)=\mathop{\mathcal L}(\frac12+it)$ is one of the simplest among them. We obtain an expression for the Riemann-Siegel function $Z(t)$ in terms of the zeros of $\mathop{\mathcal L}(s)$. Implicitly, the function $\mathop{\mathcal L}(s)$ is considered by Riemann in his paper on Number Theory. Riemann spoke of having used an expression for $Ξ(t)$ in his demonstration that most of the non-trivial zeros of the zeta function lie on the critical line. Therefore, any expression deserves a study.

math.NT↗

On the approximation of the zeta function by Dirichlet polynomials

We prove that for $s=σ+it$ with $σ\ge0$ and $0<t\le x$, we have \[ζ(s)=\sum_{n\le x}n^{-s}+\frac{x^{1-s}}{(s-1)}+Θ\frac{29}{14} x^{-σ},\qquad \frac{29}{14}=2.07142\dots\] where $Θ$ is a complex number with $|Θ|\le1$. This improves Theorem 4.11 of Titchmarsh.

math.NT↗

Density theorems for Riemann's auxiliary function

We prove a density theorem for the auxiliar function $\mathop{\mathcal R}(s)$ found by Siegel in Riemann papers. Let $α$ be a real number with $\frac12< α\le 1$, and let $N(α,T)$ be the number of zeros $ρ=β+iγ$ of $\mathop{\mathcal R}(s)$ with $1\ge β\geα$ and $0<γ\le T$. Then we prove \[N(α,T)\ll T^{\frac32-α}(\log T)^3.\] Therefore, most of the zeros of $\mathop{\mathcal R}(s)$ are near the critical line or to the left of that line. The imaginary line for $π^{-s/2}Γ(s/2)\mathop{\mathcal R}(s)$ passing through a zero of $\mathop{\mathcal R}(s)$ near the critical line frequently will cut the critical line, producing two zeros of $ζ(s)$ in the critical line.

math.NT↗

Mean Values of the auxiliary function

Let $\mathop{\mathcal R}(s)$ be the function related to $ζ(s)$ found by Siegel in the papers of Riemann. In this paper we obtain the main terms of the mean values \[\frac{1}{T}\int_0^T |\mathop{\mathcal R}(σ+it)|^2\Bigl(\frac{t}{2π}\Bigr)^σ\,dt, \quad\text{and}\quad \frac{1}{T}\int_0^T |\mathop{\mathcal R}(σ+it)|^2\,dt.\] Giving complete proofs of some result of the paper of Siegel about the Riemann Nachlass. Siegel follows Riemann to obtain these mean values. We have followed a more standard path, and explain the difficulties we encountered in understanding Siegel's reasoning.

math.NT↗

Infinite Product of the Riemann auxiliary function

We obtain the product for the auxiliary function $\mathop{\mathcal R}(s)$ and study some related functions as its phase $ω(t)$ at the critical line. The function $ω(t)$ determines the zeros of $ζ(s)$ on the critical line. We study the influence of the zeros of $\mathop{\mathcal R}(s)$ on $ω(t)$. Thus, the relationship between the zeros of $\mathop{\mathcal R}(s)$ and those of $ζ(s)$ is determined.

math.NT↗

Zeros of $\mathop{\mathcal R}(s)$ on the fourth quadrant

We show that there is a sequence of zeros of $\mathop{\mathcal R}(s)$ in the fourth quadrant. We show that the $n$-th zero $ρ_{-n}=β_{-n}+iγ_{-n}$, with $β_{-n}\sim 4π^2 n/\log^2n$ and $γ_{-n}\sim-4πn/\log n$. We give the first terms of an asymptotic development of $ρ_{-n}$ and an algorithm to calculate $ρ_{-n}$ from $n$.

math.NT↗