arXiv:0905.0830v1
Abstract
We establish that the set of pairs of real numbers such that where denotes the distance to the nearest integer, has full Hausdorff dimension in . Our proof rests on a method introduced by Peres and Schlag, that we further apply to various Littlewood-type problems
AI-generated audit
Audit summary
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
01Statements4 reported findingsCorrect
The full-dimension results for multiplicatively badly approximable pairs, their logarithmically refined and mixed -adic forms, and the dual two-variable form are correct. Theorem 4 needs only the displayed boundary correction : allowing a zero coordinate would trivially force its infimum to vanish. Its two-dimensional Peres–Schlag proof also needs a local geometric repair, supplied below, which preserves the theorem. No substantive counterexample to a central result was found.
Multiplicatively badly approximable pairs have full dimension
Pages 2 and 7–10 · Theorems 1–2 and proof of Theorem 1 · arXiv:0905.0830v1
For each fixed , the dangerous intervals around have radii proportional to . Lemma 2 makes their total loss uniformly small on every cubic block. The nested dyadic construction therefore retains a Cantor set, and its branching/separation ratio tends to one, giving full dimension in the fiber. Since the set of admissible also has dimension one, the cited slicing principle gives dimension two for the set of pairs.
The logarithmically refined fiber theorem
Page 3 and pages 6 and 10 · Theorem 3, Lemma 3, and proof reduction · arXiv:0905.0830v1
Bounded continued-fraction quotients for give uniform distribution on each denominator block and This is exactly the loss estimate needed after replacing by . The original branching argument is unchanged, so the full-dimension conclusion follows.
The mixed -adic full-dimension result
Pages 4 and 7 and 10 · Theorem 5, Lemma 4, and proof reduction · arXiv:0905.0830v1
Splitting integers by yields Thus the dangerous intervals with the mixed -adic weight satisfy the same block-loss bound as in Theorem 1. The Cantor construction gives full Hausdorff dimension, and setting gives Corollary 1.
The dual two-variable theorem needs a boundary correction
Page 4 and pages 10–11 · Theorem 4 and proof outline · arXiv:0905.0830v1
The displayed infimum must range over positive integers , or equivalently over integer pairs with . With the printed , setting and taking denominators of forces to have infimum zero. Every subsequent estimate groups pairs by and therefore already uses . Changing the boundary in the one displayed statement repairs the issue without altering any related claim.
02Proofs4 reported findingsContains incorrect or incomplete proofs
The one-dimensional Cantor construction and the logarithmic and -adic adaptations are correct. The proof outline for Theorem 4 incorrectly says that a fixed pair determines a unique integer level in the unit square and omits the resulting local strip-count calculation. Accounting for all relevant levels supplies a verified repair with the same summability bound.
The dyadic survival and mass-distribution estimates close
Pages 7–10 · equations (4.1)–(4.10) and conclusion · arXiv:0905.0830v1
Bad approximability supplies both and the uniform block sum in Lemma 2. Each retained dyadic interval loses at most a fixed small fraction to the next cubic block of dangerous sets. The construction keeps at least mutually separated children. Since and , the mass-distribution quotient tends to one. Hence the resulting set is nonempty and has Hausdorff dimension one.
All three block-sum estimates have the required uniform scale
Pages 5–7 · Lemmas 2–4 · arXiv:0905.0830v1
Lemma 2 follows by dividing the classical partial sum by the minimum on . Lemma 3 decomposes into convergent-denominator blocks; bounded partial quotients make their number and each weighted block . Lemma 4 decomposes by the exact -adic valuation and sums over . These are precisely the uniform bounds used later.
A fixed normal vector has many integer levels, not one
Pages 10–11 · proof of Theorem 4 · arXiv:0905.0830v1
For fixed positive integers , the unit square meets generally lines , not a unique line as stated. Each corresponding dangerous strip has width and intersection length at most . Since , the total area over all relevant is still . The same estimate holds locally in every retained dyadic square, with only a boundary constant. Therefore and the two-dimensional Cantor/mass-distribution construction proceeds exactly as in Theorem 1. This supplies the missing multiplicity calculation and verifies the theorem.
The convergent-index order is reversed in one sentence
Page 6 · proof of Lemma 3 · arXiv:0905.0830v1
If is the largest index with and the smallest with , then and both are comparable to . The printed chain reverses their order; it should state . The proof immediately sums from to and therefore uses the corrected order.
03Novelty0 reported findingsNo non-novelty findings
No non-novelty findings.