Abstract

Motivated by the Lester-Wigman vanishing area correlation conjecture for lattice points near the boundary of circles of growing radius, we investigate the dynamics of circle flows on tori (which are related to the motion of a charged particle in a magnetic field on a torus.) We show that an analogue of the vanishing correlation conjecture holds in this setting, i.e., we have "mixing for the area observable" despite the flow being essentially integrable. We also determine the probability density function of the areas, in global as well as local regimes.

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Audited against arXiv v1

Not a correctness certificate. A “Correct” result may include yellow typos or minor formal corrections that do not affect substantive soundness. It means this audit found no unresolved substantive error under the stated criteria; it does not replace expert scrutiny or formal verification.

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Detailed mathematical audit

Generated August 18, 2026
01Statements3 reported findingsCorrect

The correlation theorem and global distribution laws are supported. Theorem 1 proves asymptotic decorrelation in its stated joint range. Proposition 2 computes the limiting mean and variance of the area variable. Proposition 3 identifies the global limiting density from the continuum parallel-line model. A missing no-vertex-crossing hypothesis in Lemma 4 is a local formal correction and does not affect the circular-arc applications.

Theorem 1Correct

Vanishing local correlations for the lattice-circle area process

Pages 1–3 · Theorem 1 · arXiv:2607.13659v1

In the simultaneous range of radius, separation kk, and interval length specified in Theorem 1, the centered areas cut out by successive lattice-circle intersections have correlation tending to zero. The quantitative error is uniform in the admissible interval and kk ranges, with Q=min{logR,k/logk}Q=\min\{\log R,\sqrt{k}/\log k\}. The continuum comparison uses the same normalization as the discrete area variables. The standing exclusion of lattice points on the circle removes simultaneous horizontal/vertical crossings, including the minor Lemma 4 issue recorded below.

Propositions 2–3Correct

Global moments and limiting area density

Pages 3–4 and 24–29 · Propositions 2–3 · arXiv:2607.13659v1

Averaging the local continuum law over slope and intercept gives the density printed in Proposition 3. Its integral is one, and direct integration gives the mean and second moment used in Proposition 2. The discrete-to-continuum error is integrable uniformly over the circle, while the excluded low-denominator arcs have vanishing weight. Thus the moment limits and density use the same normalization as Theorem 1.

Lemma 4Minor formal correction · no status impact

The monotone-curve square count needs a no-vertex-crossing hypothesis

Page 6 · Lemma 4, second assertion · arXiv:2607.13659v1

As written for an arbitrary coordinatewise monotone curve, the assertion is false: the segment from (0,0)(0,0) to (n,n)(n,n) meets only the diagonal half-open squares, not 2n+O(1)2n+O(1) squares. The intended applications are circular arcs, and the standing assumption C(R)Z2=C(R)\cap\mathbb{Z}^2=\varnothing excludes simultaneous horizontal and vertical grid crossings. Adding that no-vertex-crossing hypothesis repairs every use without changing a main result.

02Proofs3 reported findingsCorrect

Equidistribution of boundary intersections and decorrelation. The circle is decomposed into Farey arcs according to the slope denominator. Low-height exceptional slopes have negligible total length. On every remaining short arc, rational-grid equidistribution replaces the discrete sequence of cell crossings by the continuum model, with an error uniform in the allowed separation kk. In that model the relevant parallel-line area variable has mean one half and the separated variables factor asymptotically. Summing the arc estimates proves Theorem 1; integrating the one-point formulas gives the global mean, variance, and density in Propositions 2–3.

Farey and continuum reductionCorrect and complete

Equidistribution of boundary intersections and decorrelation

Pages 9–29 · Sections 3–7 · arXiv:2607.13659v1

The circle is decomposed into Farey arcs according to the slope denominator. Low-height exceptional slopes have negligible total length. On every remaining short arc, rational-grid equidistribution replaces the discrete sequence of cell crossings by the continuum model, with an error uniform in the allowed separation kk. In that model the relevant parallel-line area variable has mean one half and the separated variables factor asymptotically. Summing the arc estimates proves Theorem 1; integrating the one-point formulas gives the global mean, variance, and density in Propositions 2–3.

Sections 5–7Correct and complete

Farey dissection, equidistribution, and global averaging

Pages 16–29 · Sections 5–7 · arXiv:2607.13659v1

Farey neighbours control how the circle crosses consecutive grid lines and isolate arcs with small rational slope denominator. The exceptional arcs satisfy the required total-length bound. On the complement, exponential-sum/equidistribution estimates are uniform in QQ and kk, and the choice Q=min{logR,k/logk}Q=\min\{\log R,\sqrt{k}/\log k\} makes every error term vanish. The continuum integral then gives decorrelation and, after one-point averaging, the global law.

Proof of Lemma 4Minor formal correction · no status impact

Simultaneous grid crossings are not counted

Page 6 · proof of Lemma 4 · arXiv:2607.13659v1

The proof adds horizontal and vertical crossings as if they were always distinct. They are distinct for the circle arcs used later because the circle contains no lattice point. Stating that restriction in the lemma makes the count and all downstream applications valid.

03Novelty0 reported findingsNo non-novelty findings

No non-novelty findings.

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Paper
arXiv:2607.13659v1
Authors listed
Matteo Bordignon, Pär Kurlberg
Audit date
August 18, 2026
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