arXiv:2401.15586v2
Abstract
We show that the statistics of the continued fraction expansion of a randomly chosen rational in the unit interval, with a fixed large denominator , approaches the Gauss-Kuzmin statistics with polynomial rate in . This improves on previous results giving the convergence without rate. As an application of this effective rate of convergence, we show that the statistics of a randomly chosen rational in the unit interval, with a fixed large denominator and prime numerator, also approaches the Gauss-Kuzmin statistics. Our results are obtained as applications of improved non-escape of mass and equidistribution statements for the geodesic flow on the space .
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Detailed mathematical audit
01Statements2 reported findingsCorrect
The quantitative continued-fraction equidistribution results, their stability for large denominator subsets, the prime-numerator consequence, and the non-escape-of-mass theorem are correct.
The continued-fraction estimates are correct
Pages 2–5 and 15–19 · Theorems 1.2–1.4 · arXiv:2401.15586v2
The geodesic-orbit estimates translate to Gauss-word frequencies and normalized continued-fraction lengths with the displayed constants. The exceptional-set count is polynomially smaller than the denominator family, so any subset of size inherits the convergence, and the prime-numerator family satisfies that size condition.
Full paper, version 2 ↗The mass and equidistribution conclusions follow with the stated threshold
Pages 6–7 and 10–15 · Theorem 1.6 and Corollary 1.7 · arXiv:2401.15586v2
The covering estimate bounds the proportion of starting points whose trajectories spend at least a fixed fraction outside a compact set. Averaging over a denominator subset of exponent leaves at least mass in the space. When , entropy rigidity identifies the full weak-star limit with Haar measure.
02Proofs2 reported findingsCorrect
The escape estimate, entropy argument, and continued-fraction deductions are correct and complete. One sentence reverses ‘upper’ and ‘lower’ but the displayed inequality and its use are correct.
An upper bound is called a lower bound
Page 13 · sentence immediately after equation (2.2) · arXiv:2401.15586v2
Equation (2.2) bounds the escaping mass from above, but the following sentence calls it a ‘lower bound’. The next line correctly subtracts it from to obtain a lower bound for compact mass. Replacing ‘lower’ by ‘upper’ is the unique correction and changes no inference.
The orbit-covering and continued-fraction steps close
Pages 10–19 · Sections 2–3 · arXiv:2401.15586v2
The continuous-time visit proportion is compared in the correct direction with the sampled flow, the covering exponent is combined with the subset cardinality before limits are taken, and the coding identities transfer the result to word frequencies and lengths without losing the stated error rate.
03Novelty0 reported findingsNo non-novelty findings
No non-novelty findings.