arXiv:2308.03049v1
Abstract
Let , let be an arbitrary norm on , and let be the best approximation vectors sequence of with respect to . We define the nth long displacement vector of to be and prove the existence of long displacement vectors who have non-typical properties, focusing on their length, direction, and congruence class.
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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
01Statements3 reported findingsCorrect
The prescribed-length, direction, and congruence construction for long displacement vectors in dimension two, together with the stated limiting-spectrum and lattice-flow consequences, is correct. The detected interval-sequence and labeling defects do not change any mathematical conclusion.
Simultaneous control of long displacement vectors
Pages 5–6 and 10–35 · Theorem 1, Theorem 2, and the inductive construction · arXiv:2308.03049v1
For an arbitrary norm on , the construction chooses successive primitive triples and keeps the associated approximation cylinders free of interior lattice points. Proposition 3 then identifies the limiting sequence as the best-approximation sequence of . Property (2.4) gives the prescribed values of , property (2.6) gives the cone and alternating-quadrant conditions, and property (2.7) gives the requested residue class. The coefficient of is , so primitivity is preserved. Since , the resulting vectors are not badly approximable. These implications establish all parts of the theorem.
Interval in the limiting Dirichlet spectrum and uncountably many convergent vectors
Pages 6–7 · Corollaries 1 and 2 · arXiv:2308.03049v1
Apply Theorem 1 with a sequence of non-degenerate closed intervals shrinking to any prescribed . The resulting long-displacement norms converge to , and the theorem supplies continuum many distinct best-approximation sequences. The eventual uniqueness of the best-approximation sequence for a fixed vector prevents this continuum from collapsing to countably many vectors. Thus lies in the limiting spectrum, and the set of Dirichlet-converging vectors is uncountable. For a diagonal ellipsoidal norm, the displayed value of agrees with the sharp Dirichlet constant, so the equality asserted in Corollary 1 follows.
Prescribed eventual height for the associated lattice trajectory
Pages 7–8 · Corollary 3 and its proof · arXiv:2308.03049v1
For , the local maxima of the first minimum along satisfy Choosing the long-displacement norms to converge to therefore makes these local maxima converge to , proving the claimed eventual compact-exhaustion threshold. The invalid displayed interval sequence has the harmless replacement recorded under Proofs.
02Proofs5 reported findingsCorrect
The reduction to an inductively constructed primitive lattice basis and the geometric cylinder-avoidance argument are correct and complete at the level required for the central results. Two local interval-sequence or labeling defects admit verified corrections and do not affect the proof status.
Cylinder exclusion identifies the limiting best approximations
Pages 9 and 11–12 · Proposition 3 and proof of Theorem 1 from Theorem 2 · arXiv:2308.03049v1
The strict growth of , strict decrease of the errors, and absence of an integer point in the interior of each approximation cylinder are exactly the defining minimality conditions for successive best approximations. If an integer pair contradicted the limiting condition, continuity would place it in the interior of the corresponding finite-stage cylinder for all sufficiently large construction stages, contradicting property (2.1). Passing properties (2.4) and (2.6) to the limit is valid because the prescribed intervals and cone are closed at the final stage.
Normalization and lattice-point selection preserve the induction
Pages 13–29 · Sections 3 and 4 · arXiv:2308.03049v1
The map fixes the denominator coordinate, sends the current primitive plane and its neighboring translate to horizontal planes, and preserves the ellipsoidal norm in the transverse coordinates. Its covolume relation follows from unimodularity. The regions and are arranged so that the relevant ellipsoidal cylinders contain no unintended points of the two adjacent lattice planes. Irrationality of the selected vertical spacing supplies infinitely many lattice candidates with every residue adjustment , while their denominators tend to infinity. These facts provide precisely the candidates used in the final induction.
Properties (2.1)–(2.7) close simultaneously
Pages 29–35 · Section 5 · arXiv:2308.03049v1
Increasing the candidate index makes arbitrarily large and arbitrarily small, preserving all earlier strict inequalities. The direction of the new error approaches the negative of the preceding error, giving the alternating-quadrant condition. Lemma 10 fixes the limiting value of inside the target interval. The adjacent-plane cylinder exclusion proves (2.1), and choosing among a complete residue block proves (2.7). The coefficient on the third basis vector proves the next triple remains a lattice basis.
The displayed interval sequence needs an arbitrary finite prefix
Pages 7–8 · first paragraph of the proof of Corollary 3 · arXiv:2308.03049v1
The proof displays the target intervals as for every . For , and for finitely many initial whenever is small, these endpoints are negative and the power is not a real interval. Choose arbitrary admissible non-degenerate intervals for those finitely many indices and use the displayed intervals once both endpoints are nonnegative (for , use any positive intervals shrinking to ). The limiting local-maximum calculation is unchanged, so no statement or downstream argument requires correction.
The table is attached to an empty numbered equation
Page 6 · empty display labeled (4) immediately before the table · arXiv:2308.03049v1
The source creates an empty equation solely to obtain label (4), then later refers to the table as equation (4). Attach the label to the table or call it “Table 1.” The four displayed constants themselves are obtained by substitution in formula (3), so this labeling defect has no mathematical effect.
03Novelty0 reported findingsNo non-novelty findings
No non-novelty findings.