\documentclass[11pt,reqno]{amsart} \usepackage[T1]{fontenc} \usepackage{lmodern} \usepackage[hmargin=1.1in,vmargin=1in]{geometry} \usepackage{mathtools,amssymb,microtype,graphicx,needspace} \usepackage[hidelinks]{hyperref} \hypersetup{pdftitle={Non-computable derivatives of the fractional-part autocorrelation}} \numberwithin{equation}{section} \newtheorem{theorem}{Theorem}[section] \newtheorem{proposition}[theorem]{Proposition} \newtheorem{lemma}[theorem]{Lemma} \newtheorem{corollary}[theorem]{Corollary} \theoremstyle{definition} \newtheorem{definition}[theorem]{Definition} \theoremstyle{remark} \newtheorem{remark}[theorem]{Remark} \newcommand{\N}{\mathbb N} \newcommand{\Q}{\mathbb Q} \newcommand{\R}{\mathbb R} \newcommand{\Z}{\mathbb Z} \newcommand{\W}{\mathcal W} \newcommand{\leT}{\leq_{\mathrm T}} \newcommand{\nleT}{\nleq_{\mathrm T}} \newcommand{\eqT}{\equiv_{\mathrm T}} \newcommand{\degT}{\deg_{\mathrm T}} \newcommand{\zerojump}{\mathbf 0'} \newcommand{\Irr}{(0,1)\setminus\Q} \newcommand{\ignore}[1]{} \title[Non-computable derivatives]{Non-computable derivatives of the\ fractional-part autocorrelation} % Authorship and affiliation are left for the authors to supply. \author{Michael Yampolsky} \date{\today} \keywords{Computable analysis, fractional-part autocorrelation, Wilton function, continued fractions, non-computable derivatives} \begin{document} \begin{abstract} We describe a natural new example of non-computability in analysis. Namely, the multiplicative autocorrelation of the fractional-part function, \[ A(x)=\int_0^\infty \{t\}\{xt\}\,\frac{dt}{t^2}, \] is computable and differentiable almost everywhere, but its finite derivative can be non-computable even for a computable $x$. We derive these results from an adaptation of our earlier work \cite{YS} on computability of Brjuno-like functions. \end{abstract} \maketitle \section*{The use of AI} The author acknowledges using an OpenAI model in writing this paper. The author has formulated the problem. The proofs are based on the author's ideas, and, in particular, an earlier work \cite{YS}. The author assumes full responsibility for the content and its correctness. \section{Introduction and main results} This paper introduces an interesting new example of a natural non-computable function of a real variable. The {\it multiplicative autocorrelation of the fractional-part function} is defined by an absolutely convergent, nonnegative integral: \begin{equation}\label{eq:A} A(x)=\int_0^\infty \{t\}\{xt\}\,\frac{dt}{t^2},\qquad x\geq 0\text{ where }\{t\}=t-\lfloor t\rfloor. \end{equation} The analytic properties of $A$ were studied by B\'aez-Duarte, Balazard, Landreau, and Saias \cite{BD,BDlong} in the context of analytic number theory. In particular, $A(x)$ is continuous and differentiable almost everywhere. Its value is effectively computable from the point of evaluation via an explicit approximation process. Yet, strikingly for such a simple-looking analytic expression, its derivative $A'(x)$ at a point $x$ may be well-defined, yet not be computable from $x$. In fact, non-computability may occur even for a computable value of $x$. The connection with our previous work flows from the results of Balazard and Martin \cite{BM}, who characterized the differentiability points of $A(x)$ through a continued-fraction series introduced by Wilton \cite{Wilton}. We combine their identities with the non-computability theorem for the signed Wilton series obtained in our paper \cite{YS}, and then refine the conclusion by constructing computable inputs. Both arguments require the same effective step: computing the correction terms that relate the Wilton series to $A'$. Before stating the theorems, let us introduce several series. For irrational $x\in(0,1)$, set \begin{equation}\label{eq:DS} D(x)=\sum_{m=1}^{\infty}\frac{\{mx\}-1/2}{m},\qquad S(x)=\sum_{m=1}^{\infty}\frac{\tau(m)}m\sin(2\pi mx), \end{equation} where $\tau(m)$ is the number of positive divisors of $m$. %These are ordinary convergent-series values, not values assigned by a summability method. Further, to define the Wilton function, set \[ T(x)=\{1/x\},\qquad x_n=T^n(x),\qquad \beta_{-1}(x)=1,\quad \beta_{n-1}(x)=x_0\cdots x_{n-1}\quad(n\geq1), \] and let \begin{equation}\label{eq:W} W(x)=\sum_{n=0}^{\infty}(-1)^n\beta_{n-1}(x)\log\frac1{x_n}. \end{equation} %All logarithms are natural. We denote by $\W$ the set of \emph{Wilton numbers}, namely the irrational $x\in(0,1)$ for which \eqref{eq:W} converges. Absolute convergence defines the smaller class of {\it Brjuno numbers} which play a special role in the study of small-divisor problems in holomorphic dynamics \cite{yoccoz1995}. We use the Cauchy representation of real numbers. {\it An oracle for $x$} is a function which returns rational approximations to $x$ with error less than $2^{-n}$ on input $n$. The notation $y\leT x$ means that one oracle algorithm computes $y$ from every Cauchy name of this fixed $x$. A function on a specified domain is {\it computable} if one oracle algorithm works for every input in that domain. In particular, $F(x)\nleT x$ is a pointwise obstruction, stronger than the failure of a single algorithm to work uniformly on the whole domain. The first result is a direct corollary of the signed Wilton theorem of \cite{YS}, once we have made effective the known analytic identities for $A'(x)$. \begin{theorem}\label{thm:main} The function $A$ is computable on $[0,\infty)$. Every nonempty open interval $I\subset(0,1)$ contains a point $x\in\W$ at which $A'(x)$ exists as a finite real number and \begin{equation}\label{eq:noncomputability} A'(x)\nleT x,\qquad D(x)\nleT x,\qquad S(x)\nleT x,\qquad W(x)\nleT x. \end{equation} Moreover, at every $x\in\W$, the four quantities are mutually computable relative to $x$: uniformly on this domain, \begin{equation}\label{eq:joins} x\oplus A'(x)\eqT x\oplus D(x)\eqT x\oplus S(x)\eqT x\oplus W(x). \end{equation} \end{theorem} The non-computability input here is precisely \cite[Theorems~5.1 and~5.2]{YS}, applied to their second Wilton function. Theorem~\ref{thm:main} does not, by itself, assert that the input value $x$ is computable. Our second result supplies computable $x$ and specifies the amount of information in the four values. A real number is \emph{limit-computable} if it is the limit of a computable sequence of rationals, without a required computable rate of convergence. It is \emph{left-computably enumerable (left-c.e.)} if it admits such a nondecreasing approximation; right-c.e. is defined using nonincreasing approximations. A c.e. Turing degree is the degree of a computably enumerable subset of $\N$, and $\zerojump$ denotes the degree of the halting problem. \begin{theorem}[{\bf Computable-input refinement}]\label{thm:refined} Let $r\in(0,1)$ be limit-computable, and let $I\subset(0,1)$ be a nonempty open interval with rational endpoints. There is a computable $x\in I\cap\W$ such that $A'(x)$ exists and \begin{equation}\label{eq:degrees} A'(x)\eqT D(x)\eqT S(x)\eqT W(x)\eqT r. \end{equation} More precisely, the construction gives \begin{equation}\label{eq:affineW} W(x)=(\log2)r+c \end{equation} with $c$ computable. Both $x$ and $c$ are computable uniformly from $I$ and a program producing a convergent rational approximation to $r$. If the supplied approximation has finite total variation, then $x$ can be chosen Brjuno. In particular, this applies to a nondecreasing approximation. \end{theorem} \begin{corollary}\label{cor:brjuno} In every nonempty open subinterval of $(0,1)$ there is a computable Brjuno number $x$ for which $A'(x),D(x),S(x),W(x)$ are all finite and non-computable. They can be chosen to have any prescribed nonzero c.e. Turing degree. \end{corollary} \Needspace{8\baselineskip} \begin{theorem}[{\bf Full degree spectrum}]\label{thm:spectrum} For every nonempty open interval $I\subset(0,1)$ and each $F\in\{A',D,S,W\}$, \begin{equation}\label{eq:spectrum} \bigl\{\degT F(x):x\in I\cap\W\text{ is computable}\bigr\} =\bigl\{\mathbf d:\mathbf d\leq\zerojump\bigr\}. \end{equation} Each degree on the right is realized simultaneously by the four quantities at a single computable point in $I$. \end{theorem} The full spectrum concerns Wilton points, not necessarily Brjuno points. Computable Brjuno points already suffice to realize all c.e. degrees, including the computable degree. %At the Brjuno points in Corollary~\ref{cor:brjuno}, the Wilton series is absolutely convergent; %no assertion of absolute convergence is being made for $D$ or $S$. Section~\ref{sec:background} presents the basic analytic properties of $A$. Sections~\ref{sec:effective} and~\ref{sec:transfer} prove the common reduction \begin{equation}\label{eq:lead-reduction} A'(x)=C(x)-\frac{W(x)}{2x}\qquad(x\in\W), \end{equation} where $C$ is computable from $x$. Section~\ref{sec:YS} then proves the direct corollary of \cite{YS}. Section~\ref{sec:refinement} supplies the adapted realization argument, and Section~\ref{sec:consequences} deduces the degree spectrum and the one-sided computability statements. \section{Basic properties of the autocorrelation} \label{sec:background} \subsection{Reciprocity and the Hilbert-space interpretation} Near zero the integrand in \eqref{eq:A} equals $x$, and near infinity it is bounded by $t^{-2}$, so $A(x)$ is finite for every $x\geq0$. A change of variables gives \begin{equation}\label{eq:reciprocity} A(x)=xA(1/x)\qquad(x>0). \end{equation} This identity will reduce computation on $[0,\infty)$ to computation on $[0,1]$. The name ``autocorrelation'' has a literal Hilbert-space meaning. Let $f(t)=\{t\}$. In the Hilbert space $L^2((0,\infty),dt/t^2)$ we have \[ A(x)=\langle f,f(x\,\cdot)\rangle,\qquad \|f(x\,\cdot)\|_2^2=x\|f\|_2^2. \] Cauchy--Schwarz therefore gives \begin{equation}\label{eq:CS} 00),\qquad A(1)=\log(2\pi)-\gamma, \end{equation} where $\gamma$ is Euler's constant. The value at $1$ follows by integration over successive unit intervals and Stirling's formula; see \cite[Propositions~85 and~87]{BDlong}. Our algorithm below computes $A(1)$ directly from the integral and does not require this special-value formula. \subsection{Regularity and differentiability} Balazard and Martin prove that the global modulus of continuity \[ \omega_A(h)=\sup_{\substack{x,y\geq0\\|x-y|\leq h}}|A(x)-A(y)| \] satisfies \begin{equation}\label{eq:sharp-modulus} \omega_A(h)=\frac12 h\log(1/h)+O(h)\qquad(h\downarrow0); \end{equation} see \cite[Proposition~31]{BM}. This describes the regularity of $A$, but we do not use the unspecified constant in the $O(h)$ term to compute it. Proposition~\ref{prop:Acomputable} supplies an explicit modulus and an effective truncation bound for that purpose. At a positive rational $p/q$ in lowest terms, $A$ has a logarithmic cusp: \begin{equation}\label{eq:cusp} A(p/q+h)-A(p/q) =\frac{|h|\log|h|}{2p}+O_{p,q}(|h|)\qquad(h\to0), \end{equation} by \cite[Proposition~98]{BDlong}. Thus every positive rational is a strict local maximum, with infinite one-sided slopes. These singularities explain the cusps visible in Figure~\ref{fig:A}. For irrational $x\in(0,1)$, there is an exact criterion: $A'(x)$ exists as a finite real number if and only if $x\in\W$ \cite[Theorem~1 and Proposition~30]{BM}. The Wilton set has full Lebesgue measure in $(0,1)$, so $A$ is differentiable almost everywhere there -- and (\ref{eq:reciprocity}) extends this conclusion to $(0,\infty)$. %The pointwise criterion, rather than the almost-everywhere assertion, guarantees %existence at the inputs used in our non-computability arguments. The identities for the derivative values are stated in Theorem~\ref{thm:BM}. \begin{figure}[tbp] \centering \includegraphics[width=0.94\textwidth]{autocorrelation_graph.pdf} \caption{The autocorrelation $A$ on $[0,2]$. Values at mesh points $p/2400$ were computed using the finite cotangent-sum formula of \cite[Proposition~89]{BDlong} and joined. The graph illustrates the rational cusps.} \label{fig:A} \end{figure} \section{Effective evaluation of the autocorrelation and the correction} \label{sec:effective} \subsection{Computability of the autocorrelation} We first evaluate truncated integrals at rational arguments, then use an explicit modulus to pass to arbitrary Cauchy names. \begin{proposition}\label{prop:Acomputable} The function $A$ is computable on $[0,\infty)$. On $[0,1]$, one has $0\leq A(x)\leq2$, and for each integer $M\geq1$, \begin{equation}\label{eq:Amodulus} |A(x)-A(y)|\leq |x-y|(2+2\log M)+\frac2M, \qquad 0\leq x,y\leq1. \end{equation} \end{proposition} \begin{proof} Let $A_M(x)$ denote the integral in \eqref{eq:A} truncated at $M$. Its tail lies in $[0,1/M]$, uniformly in $x$. For rational $x\in(0,1]$, split $[1,M]$ at the finitely many rational points where $t$ or $xt$ is integral. On an intervening interval, \[ \frac{\{t\}\{xt\}}{t^2} =\frac{(t-j)(xt-k)}{t^2} =x-\frac{k+jx}{t}+\frac{jk}{t^2}. \] Integrating uses only rational arithmetic and logarithms of positive rationals. The contribution of $(0,1)$ is $x$, and $A(0)=0$. Thus $A$ is uniformly computable at rational inputs. To pass to arbitrary Cauchy names, suppose $0\leq x1/(B+1)$ for every $n$, and the terms in \eqref{eq:W} are bounded in absolute value by $\log(B+1)2^{-\lfloor n/2\rfloor}$. The series for $W$ then has an effective tail bound, and all four quantities in Theorem~\ref{thm:main} are computable relative to $x$, uniformly with the bound $B$. For example, at $\omega=(\sqrt5-1)/2$, the functional equation $W(\omega)=\log(1/\omega)-\omega W(\omega)$ gives \[ W(\omega)=\frac{\log(1/\omega)}{1+\omega}, \] so $A'(\omega)$ is computable as well. At a point furnished by Theorem~\ref{thm:main}, or by Theorem~\ref{thm:refined} with non-computable $r$, every finite partial sum of $D,S,W$ is computable from $x$, and so are the difference quotients \[ \frac{A(x+2^{-n})-A(x)}{2^{-n}}. \] All the relevant limits exist. None of these approximation sequences can have a convergence modulus computable from $x$, since such a modulus would compute the limit. In contrast, the correction series $G$ and the comparison series $H$ have the explicit effective tails \eqref{eq:Gtail} and \eqref{eq:tailbounds} on every irrational input, independently of the convergence of $W$. This is the precise effective distinction behind both the direct corollary and its refinement. Knowing only that two functions differ by a bounded, or even continuous, function would not establish these computability reductions. The degree-spectrum theorem does not say that differentiation creates non-computability at every computable point, nor that $A$ is nowhere differentiable. It identifies all possible degrees of its finite derivatives at computable differentiability points, while the Brjuno examples show that absolute convergence of the Wilton series alone does not make its sum computable. The example thus separates three issues within a single classical function: computability of its values, existence of its derivative, and computability of that derivative from its argument. Its significance is not an artificially chosen non-computable constant in the definition of $A$, but the arithmetic information exposed by differentiation of a computable correlation integral. } \begin{thebibliography}{99} \bibitem{BD} L.~B\'aez-Duarte, M.~Balazard, B.~Landreau, and E.~Saias, \emph{\'Etude de l'autocorr\'elation multiplicative de la fonction ``partie fractionnaire''}, Ramanujan J. \textbf{9} (2005), 215--240. \href{https://doi.org/10.1007/s11139-005-0834-4}{doi:10.1007/s11139-005-0834-4}. \bibitem{BDlong} L.~B\'aez-Duarte, M.~Balazard, B.~Landreau, and E.~Saias, \emph{Sur l'autocorr\'elation multiplicative de la fonction ``partie fractionnaire''}, detailed companion calculations (2003), \href{https://arxiv.org/abs/math/0306251}{arXiv:math/0306251}. Proposition numbers cited in the text refer to this version. \bibitem{BM12} M.~Balazard and B.~Martin, \emph{Comportement local moyen de la fonction de Brjuno}, Fund. 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