arXiv:2606.27034v2

Averaged Fourier Estimates and Dyadic Approximation on the Cantor set

Prasuna Bandi

math.NTmath.DS11J8328A8011K6037A45

Abstract

Let CC be the middle-third Cantor set and let μμ be the natural Cantor probability measure. Let γ=log2log3. γ=\frac{\log2}{\log3}. The two main results of this paper are μ{xC:2nx<nτ for infinitely many n}=0 for τ>2γ. μ\{x\in C:\|2^n x\|<n^{-τ}\text{ for infinitely many }n\}=0 \qquad \text{ for } τ>2-γ. and μ{xC:2nx<nτ for infinitely many n}=1 for τ<1γ2. μ\{x\in C:\|2^n x\|<n^{-τ}\text{ for infinitely many }n\}=1 \qquad \text{ for } τ<\frac{1-γ}{2}. These results give new progress toward Velani's conjecture on zero-one law for dyadic approximation in the middle-third Cantor set.

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Audit summary

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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Detailed mathematical audit

Generated August 15, 2026
01Statements2 reported findingsCorrect

The convergence threshold τ>2γ\tau>2-\gamma and the full-measure threshold 0<τ<(1γ)/20<\tau<(1-\gamma)/2 are correct for the stated Ahlfors-regular measures with Fourier decay along powers of three. The auxiliary Fourier and transfer estimates support both conclusions.

Theorem 1Correct

Convergence result above the threshold 2γ2-\gamma

Pages 3 and 11–12 · Theorem 1 and its proof · arXiv:2606.27034v2

With β=1γ\beta=1-\gamma, the coarse target of radius NβN^{-\beta} has averaged mass O(N1β)=O(Nγ)O(N^{1-\beta})=O(N^\gamma). The coarse-to-fine transfer bounds each fine event of radius nτn^{-\tau} by the factor (Nτ/Nβ)γ=Nγ(τβ)(N^{-\tau}/N^{-\beta})^\gamma=N^{-\gamma(\tau-\beta)} times its coarse counterpart on N<n2NN<n\leq2N. The dyadic block sum is therefore O(Nγ(1+βτ))O(N^{\gamma(1+\beta-\tau)}), which is summable over dyadic NN exactly when τ>1+β=2γ\tau>1+\beta=2-\gamma. Borel–Cantelli then gives the stated zero-measure conclusion.

Full paper, version 2
Theorem 2Correct

Divergence result below the threshold (1γ)/2(1-\gamma)/2

Pages 3 and 13–15 · Theorem 2 and its proof · arXiv:2606.27034v2

For the smoothed counting function, the mean over N<n2NN<n\leq2N is N1τ\asymp N^{1-\tau} and its second moment has error O(N1+γ)O(N^{1+\gamma}). Chebyshev's inequality therefore gives an exceptional-measure bound of order N1+γ+2τN^{-1+\gamma+2\tau}. This is summable on dyadic scales when 2τ<1γ2\tau<1-\gamma, forcing infinitely many solutions for almost every point. The smoothing functions are nested inside the desired target intervals, so the conclusion transfers to the original limsup set.

Full paper, version 2
02Proofs5 reported findingsCorrect

The cosine-product averaging, linear and bilinear Fourier estimates, Ahlfors-regular transfer, and first- and second-moment arguments are correct and complete. One fixed-constant scope extension should be stated explicitly, and several notation slips should be corrected; all have unambiguous repairs and do not affect the overall correctness status.

Lemmas 3–8Correct and complete

Fourier averaging estimates

Pages 4–8 · Lemmas 3–8 · arXiv:2606.27034v2

Expanding the ternary Riesz product reduces the relevant sums to cosine averages indexed by signed ternary combinations. Orthogonality controls the multiplicities, and the hypotheses μ^(3k)3γk|\widehat\mu(3^k)|\ll3^{-\gamma k} then give the stated linear and bilinear estimates after the low- and high-frequency ranges are separated. The powers of HH, the choice 3KH<3K+13^K\leq H<3^{K+1}, and the resulting HγH^\gamma loss are consistent throughout.

Lemmas 9–12 and Theorems 1–2Correct and complete

Moment estimates and coarse-to-fine transfer

Pages 8–15 · Lemmas 9–12 and proofs of Theorems 1–2 · arXiv:2606.27034v2

The Fourier majorants and minorants have the required coefficient bounds, Ahlfors regularity converts coarse intervals to fine intervals uniformly, and the diagonal and off-diagonal contributions to the second moment have the stated orders. The convergence proof and the variance calculation then yield exactly the threshold exponents in the two theorems. No omitted case or unjustified limiting step was found.

Lemma 11 as used in Theorem 1Minor formal correction

The coarse first-moment statement should allow a fixed multiplicative constant

Pages 10–11 · Lemma 11 and proof of Theorem 1 · arXiv:2606.27034v2

Lemma 11 is stated for δN=Nβ\delta_N=N^{-\beta}, while the proof of Theorem 1 applies it to An(2δN)A_n(2\delta_N). The lemma should be stated for δN=cNβ\delta_N=cN^{-\beta} with any fixed c>0c>0, or the proof should repeat its estimate for c=2c=2. The same Fourier argument works verbatim: only the main-term constant changes, and the coefficient bound is uniform. This is a readily verified scope correction and does not affect either theorem.

Lemmas 4, 7, and 8Typos

Three local notation and cross-reference slips

Pages 4 and 6–7 · Lemmas 4, 7, and 8 · arXiv:2606.27034v2

In the induction step of Lemma 4, the two occurrences of 3a+L13^{a+L-1} inside the translated arguments should be 3a+L1ε3^{a+L-1}\varepsilon; the following cosine factor already contains ε\varepsilon and makes the intended terms clear. Lemmas 7 and 8 say “By Lemma 3” at the point where they apply the averaging result of Lemma 4; both references should be to Lemma 4.

Lemmas 10 and 12Typos

Inconsistent coefficient and radius notation

Pages 8–11 · Lemmas 10 and 12 · arXiv:2606.27034v2

Lemma 10 occasionally writes coefficients as a,R,y±a_{\ell,R,y}^{\pm} although they were defined as a,R±a_{\ell,R}^{\pm}; the unused subscript yy should be removed. Lemma 12 defines the radius ρ\rho and then writes B(xp,ρ)B(x_p,\rho_*) twice; those occurrences should read B(xp,ρ)B(x_p,\rho). The surrounding definitions determine each correction uniquely.

03Novelty0 reported findingsNo non-novelty findings

No non-novelty findings.

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Paper
arXiv:2606.27034v2
Authors listed
Prasuna Bandi
Audit date
August 15, 2026
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