arXiv:1204.2561v1
Abstract
We prove a conjecture due to Stephen Harrap on inhomogeneous linear Diophantine approximation related to sets.
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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
01Statements2 reported findingsCorrect
The nonemptiness and full-Hausdorff-dimension conclusions for the weighted twisted set are correct; the definition contains a harmless repeated coordinate.
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 of the children meet a new resonance strip, leaving a positive branching Cantor set. The transference bound (1) sends its uniform dual separation to , and the branching estimate tends to ambient dimension two as .
Full paper, version 1 ↗The second inhomogeneous coordinate is a typo
Page 1 · displayed definition of · arXiv:1204.2561v1
The second term is printed ; it must be . 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.
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 translates and using central symmetry forces . Each of the two coordinate-dominant subsequences inherits the same bound, which limits the number of resonances in one scale block by .
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 and per resonance, combined with lacunarity, are smaller than the available children for large .
03Novelty0 reported findingsNo non-novelty findings
No non-novelty findings.