Abstract

We prove a conjecture due to Stephen Harrap on inhomogeneous linear Diophantine approximation related to BAD(α,β){\rm BAD}(α,β) sets.

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Audit summary

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.

Current report

Detailed mathematical audit

Generated August 20, 2026
01Statements2 reported findingsCorrect

The nonemptiness and full-Hausdorff-dimension conclusions for the weighted twisted set are correct; the definition contains a harmless repeated coordinate.

Main theoremCorrect

The weighted twisted set has full dimension

Pages 1-5 · theorem and Sections 2-3 · arXiv:1204.2561v1

The best-approximation sequence splits into two families with lacunarity after at most 28 terms. At each anisotropic subdivision, only O(R2logR)O(R^2\log R) of the R3R^3 children meet a new resonance strip, leaving a positive branching Cantor set. The transference bound (1) sends its uniform dual separation to BADΘ(2/3,1/3)\mathrm{BAD}_\Theta(2/3,1/3), and the branching estimate tends to ambient dimension two as RR\to\infty.

Full paper, version 1
Definition of $\mathrm{BAD}_\Theta$Typo · no status impact

The second inhomogeneous coordinate is a typo

Page 1 · displayed definition of BADΘ(α,β)\mathrm{BAD}_\Theta(\alpha,\beta) · arXiv:1204.2561v1

The second term is printed qθ2η1\|q\theta_2-\eta_1\|; it must be qθ2η2\|q\theta_2-\eta_2\|. The vector notation, every later dual form, and the two-coordinate conclusion uniquely determine this correction.

02Proofs2 reported findingsCorrect

The lacunarity count, resonance-strip estimate, nested construction, and transference step are correct and complete.

Equations (3)-(6)Correct and complete

The best-approximation families are uniformly lacunary

Pages 2-3 · equations (3)-(6) · arXiv:1204.2561v1

Partitioning the annular difference of two weighted approximation bodies into 2×282\times28 translates and using central symmetry forces Mν+282MνM_{\nu+28}\geq2M_\nu. Each of the two coordinate-dominant subsequences inherits the same bound, which limits the number of resonances in one scale block by O(logR)O(\log R).

Section 3Correct and complete

The dangerous-child counts leave a nonempty full-dimension construction

Pages 3-5 · equations (9)-(13) and final count · arXiv:1204.2561v1

For the first family, fixing the second coordinate confines every dangerous child to a horizontal interval of controlled length; the second family is symmetric with the coordinates exchanged. The resulting bounds 5R25R^2 and 6R26R^2 per resonance, combined with lacunarity, are smaller than the R3R^3 available children for large RR.

03Novelty0 reported findingsNo non-novelty findings

No non-novelty findings.

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Paper
arXiv:1204.2561v1
Authors listed
Nikolay G. Moshchevitin
Audit date
August 20, 2026
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