m -point correlations of the fractional parts of αnθ

abstract: Let $m\geq 3$, we prove that $(\alpha n^\theta\bmod 1)_{n>0}$ has Poissonian $m$-point correlation for all $\alpha>0$, provided $\theta<\theta_m$, where $\theta_m$ is an explicit bound which goes to $0$ as $m$ increases. This work builds on the method developed in Lutsko-Sourmelidis-Technau (2021), and introduces a new combinatorial argument for higher correlation levels, and new Fourier analytic techniques. A key point is to introduce an `extra' frequency variable to de-correlate the sequence variables and to eventually exploit a repulsion principle for oscillatory integrals. Presently, this is the only positive result showing that the $m$-point correlation is Poissonian for such sequences.

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Publication Details

Journal
American Journal of Mathematics
Published
2026-03-31
DOI
https://doi.org/10.1353/ajm.2026.a986600
Primary Topic
Analytic Number Theory Research
Type
article
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article

m -point correlations of the fractional parts of αnθ

Christopher Lutsko, Niclas Technau
American Journal of Mathematics
Analytic Number Theory Research
article

m -point correlations of the fractional parts of αnθ

Christopher Lutsko, Niclas Technau
article en

Abstract

abstract: Let $m\geq 3$, we prove that $(\alpha n^\theta\bmod 1)_{n>0}$ has Poissonian $m$-point correlation for all $\alpha>0$, provided $\theta<\theta_m$, where $\theta_m$ is an explicit bound which goes to $0$ as $m$ increases. This work builds on the method developed in Lutsko-Sourmelidis-Technau (2021), and introduces a new combinatorial argument for higher correlation levels, and new Fourier analytic techniques. A key point is to introduce an `extra' frequency variable to de-correlate the sequence variables and to eventually exploit a repulsion principle for oscillatory integrals. Presently, this is the only positive result showing that the $m$-point correlation is Poissonian for such sequences.

American Journal of MathematicsVol. 148(2)
Openalex Percentile: Top 17%
Analytic Number Theory Research
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