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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Audited against arXiv v2

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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Generated August 18, 2026
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.

Theorem 2.1 and Theorem ACorrect

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 BVBVLL^\infty mixing controls the separated terms, Lemma 2.3 and hypotheses (2.1)–(2.2) give a relative variance O(nη)O(n^{-\eta}) for some η>0\eta>0, and the subsequence argument plus continuous mean scaling yields the all-nn, all-s>0s>0 conclusion. The dimension inequalities in Theorem A permit parameters γ<2βCμ1,μ2\gamma<2-\beta C_{\mu_1,\mu_2} and α<2γ\alpha<2\gamma exactly when β(2Cμ1,μ2Cμi)<2\beta(2C_{\mu_1,\mu_2}-C_{\mu_i})<2 for i=1,2i=1,2; hence the printed range 0<β<2/Cmax0<\beta<2/C_{\max} is sufficient. The local notation corrections reported in Part 2 do not alter this argument.

Full paper, version 2
Theorem BCorrect

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 n2μ(B(x,s/nβ))dμ(x)n^2\int\mu(B(x,s/n^\beta))\,d\mu(x), while the four-index decomposition in Section 4 controls the well-separated, zero-gap, one-gap, and two-gap configurations. The assumptions βCμ<2\beta C_\mu<2, β(CμDμ)<1\beta(C_\mu-D_\mu)<1, and β(CμFμ)<1\beta(C_\mu-F_\mu)<1 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
Corollaries 1.5 and 1.6Incorrect

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 I=[0,1]I=[0,1] and use the four partition intervals P1=[0,1/4]P_1=[0,1/4], P2=[1/4,1/2]P_2=[1/4,1/2], P3=[1/2,3/4]P_3=[1/2,3/4], and P4=[3/4,1]P_4=[3/4,1]. Define T(x)={1/22x,xP1,2x1/2,xP2,2x1/2,xP3,5/22x,xP4.T(x)=\begin{cases}1/2-2x,&x\in P_1,\\2x-1/2,&x\in P_2,\\2x-1/2,&x\in P_3,\\5/2-2x,&x\in P_4.\end{cases} The formulas agree at common endpoints. Every branch is C1C^1, has T=2|T'|=2, zero distortion, and image diameter 1/21/2; each image is a union of partition elements. Thus TT satisfies Definition 1.4 with attractor II. Lebesgue measure is invariant with density ρ=1\rho=1, but the two halves [0,1/2][0,1/2] and [1/2,1][1/2,1] are invariant mixing components. Conditional on either half, the invariant density is 22, so the single-orbit numerator divided by n2βn^{2-\beta} tends to 4s4s, not the 2s2s asserted by Corollary 1.6. For two Lebesgue-typical points, the corresponding normalized limit is 4s4s when the points lie in the same component and 00 when they lie in opposite components, rather than the constant 2s2s 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.

Proofs of Corollaries 1.5 and 1.6Incorrect as written · verified repair

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 BVBVLL^\infty 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 BVBVLL^\infty 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
Lemma 2.2(b)Minor formal correction

The strict endpoint inequality should be non-strict

Page 11 · Lemma 2.2(b) and its proof · arXiv:2606.17880v2

The lemma concludes β<(2γ)/Cμ1,μ2\beta<(2-\gamma)/\underline C_{\mu_1,\mu_2} from (2.1), but its proof yields only β(2γ)/Cμ1,μ2\beta\leq(2-\gamma)/\underline C_{\mu_1,\mu_2}. Equality can occur: for μ1=μ2\mu_1=\mu_2 equal to Lebesgue measure, Cμ1,μ2=1\underline C_{\mu_1,\mu_2}=1 and n2μ1(B(x,s/nβ))dμ2(x)n2βn^2\int\mu_1(B(x,s/n^\beta))\,d\mu_2(x)\asymp n^{2-\beta}, so (2.1) holds with γ=2β\gamma=2-\beta. Replace << by \leq in part (b). This endpoint statement is not used in deriving Theorem A, which uses parts (a) and (c), so no main result changes.

Proof of Theorem 2.1Typo

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 i,ji,j, but the lower interpolation displays suddenly write iji\ne j, and the concluding display repeats that restriction. Replace each 0ijmK0\leq i\ne j\leq m^K there by 0i,jmK0\leq i,j\leq m^K, 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.

Proof of Theorem BTypo

The final variance estimate cites the wrong exponent label

Page 38 · Equations (4.9)–(4.10) and the final choice of δ\delta · arXiv:2606.17880v2

Proposition 4.1 supplies the well-separated error exponent ϵ2\epsilon_2, while Proposition 4.7 supplies ϵ8\epsilon_8. Equation (4.9) and the final line instead use ϵ3\epsilon_3 in place of ϵ2\epsilon_2. Replace the exponent in (4.9) by min{ϵ2,ϵ8,1}\min\{\epsilon_2,\epsilon_8,1\} and take δ\delta using min{ϵ1,ϵ2,ϵ8,1}\min\{\epsilon_1,\epsilon_2,\epsilon_8,1\}. 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.

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Paper
arXiv:2606.17880v2
Authors listed
Simon Baker, Mike Todd
Audit date
August 18, 2026
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