arXiv:2606.17880v2
Abstract
We study the pair correlation statistics of orbits generated by maps on the interval. We show that under suitable mixing and multifractal assumptions, the pair correlation statistics of an orbit will almost surely exhibit the same asymptotic behaviour as a suitable sequence of i.i.d. random variables. We will also show that, under suitable hypotheses, the pair correlation statistics defined by two orbits will almost surely exhibit the same behaviour as two suitable sequences of i.i.d. random variables. Specific dynamical systems to which our results apply to include Gibbs-Markov maps and the Gauss map. We also give an example of a slowly mixing system for which the pair correlation statistics of an orbit almost surely behave distinctly to an i.i.d. sequence.
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Detailed mathematical audit
01Statements3 reported findingsContains wrong statements
The conditional two-orbit and one-orbit limit theorems are correct under their printed mixing, dimension, early-return, and scaling hypotheses. The two advertised Gibbs–Markov corollaries are false for the class defined in the paper, because Definition 1.4 does not impose irreducibility or mixing. A piecewise linear map with two invariant mixing components satisfies that definition but gives component-dependent pair-correlation limits, contradicting both corollaries.
Two-orbit pair-correlation limit under the stated quantitative hypotheses
Pages 7 and 10–18 · Theorem A and Theorem 2.1 · arXiv:2606.17880v2
The second-moment decomposition separates two large time gaps, two short gaps, and the two half-separated regimes. Exponential – mixing controls the separated terms, Lemma 2.3 and hypotheses (2.1)–(2.2) give a relative variance for some , and the subsequence argument plus continuous mean scaling yields the all-, all- conclusion. The dimension inequalities in Theorem A permit parameters and exactly when for ; hence the printed range is sufficient. The local notation corrections reported in Part 2 do not alter this argument.
Full paper, version 2 ↗Single-orbit pair-correlation limit under mixing and recurrence hypotheses
Page 9 and Sections 3–4 · Theorem B · arXiv:2606.17880v2
The dyadic conditioning in Section 3 replaces moving balls by interval indicators at a smaller scale. The first moment is asymptotic to , while the four-index decomposition in Section 4 controls the well-separated, zero-gap, one-gap, and two-gap configurations. The assumptions , , and make every exceptional contribution lower order. The resulting summable-subsequence estimate and continuous mean scaling prove the stated almost-sure limit. The exponent-label typo reported in Part 2 has a unique mechanical correction and does not affect the theorem.
Full paper, version 2 ↗The defined Gibbs–Markov class includes nonmixing maps for which both limits fail
Pages 7–9 · Definition 1.4 and Corollaries 1.5–1.6; pages 40–41 · their proofs · arXiv:2606.17880v2
Let and use the four partition intervals , , , and . Define The formulas agree at common endpoints. Every branch is , has , zero distortion, and image diameter ; each image is a union of partition elements. Thus satisfies Definition 1.4 with attractor . Lebesgue measure is invariant with density , but the two halves and are invariant mixing components. Conditional on either half, the invariant density is , so the single-orbit numerator divided by tends to , not the asserted by Corollary 1.6. For two Lebesgue-typical points, the corresponding normalized limit is when the points lie in the same component and when they lie in opposite components, rather than the constant asserted by Corollary 1.5. Repair classification: add a mixing or primitive Markov hypothesis and specify the associated mixing acip; under that restriction the corollaries follow from Theorems A and B as claimed.
02Proofs4 reported findingsContains incorrect or incomplete proofs
The proofs of the conditional limit theorems are complete after three local notation corrections. The proofs of the Gibbs–Markov corollaries, however, invoke mixing and recurrence properties that do not follow from the paper's own Definition 1.4; the explicit two-component map in Part 1 shows that this is a substantive and conclusion-changing hypothesis failure.
Mixing is asserted for a class that does not require it
Pages 40–41 · proofs of Corollaries 1.5 and 1.6 · arXiv:2606.17880v2
The proof says that every map satisfying Definition 1.4 has exponential – mixing, and then invokes the four-mixing and early-return inputs. Definition 1.4 contains expansion, Markov, distortion, and big-image conditions but no irreducibility, aperiodicity, or mixing condition. The two-component counterexample in Part 1 satisfies every displayed defining condition and preserves Lebesgue measure, yet it is not mixing and violates both conclusions. The cited Gibbs–Markov results apply in their mixing setting and cannot supply a missing hypothesis in the paper's broader definition. The repair is verified after adding exponential – mixing to Corollary 1.5 and, for Corollary 1.6, exponential four-mixing and the stated early-return estimate; Theorems A and B plus Lemma 5.1 then give the printed limits.
Holland–Nicol–Török, Gibbs–Markov recurrence estimate ↗The strict endpoint inequality should be non-strict
Page 11 · Lemma 2.2(b) and its proof · arXiv:2606.17880v2
The lemma concludes from (2.1), but its proof yields only . Equality can occur: for equal to Lebesgue measure, and , so (2.1) holds with . Replace by in part (b). This endpoint statement is not used in deriving Theorem A, which uses parts (a) and (c), so no main result changes.
The all-integer lower interpolation accidentally excludes equal time indices
Pages 13–14 · lower-bound interpolation following Equation (2.5) · arXiv:2606.17880v2
The two-orbit count in Theorem 2.1 and Equation (2.5) ranges over all pairs , but the lower interpolation displays suddenly write , and the concluding display repeats that restriction. Replace each there by , and make the same correction in the concluding display. Monotonicity of the unrestricted count gives the displayed lower bound directly, so the intended correction is unique and no estimate changes.
The final variance estimate cites the wrong exponent label
Page 38 · Equations (4.9)–(4.10) and the final choice of · arXiv:2606.17880v2
Proposition 4.1 supplies the well-separated error exponent , while Proposition 4.7 supplies . Equation (4.9) and the final line instead use in place of . Replace the exponent in (4.9) by and take using . These are exactly the exponents furnished by the immediately preceding estimates, so the correction is mechanical and preserves a positive decay rate.
03Novelty0 reported findingsNo non-novelty findings
No non-novelty findings.