arXiv:2401.00614v3
Abstract
In this paper we study the classical Schmidt game on two families of sets: one related to frequencies of digits in base- expansions, and one connected to the set of the badly approximable numbers. Namely, we describe some nontrivial winning and losing parameters for these sets.
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Proof lineage
On Nontrivial Winning and Losing Parameters of Schmidt Games
A statement-restricted graph for arXiv:2401.00614v3. It traces the uniform-distribution, Schmidt-game, Hausdorff-dimension, and Borel-determinacy results actually imported by the v3 proofs. Theorem 2.6 is marked self-contained. Contextual citations, an earlier bound that is not used, and the different determinacy citation added only in the later journal version are excluded.
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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.
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Detailed mathematical audit
01Statements3 reported findingsCorrect
The stated winning and losing regions for digit-frequency sets and the two fixed-constant badly approximable sets are correct. The proof of the losing region for the base- set omits the rational- case, and an auxiliary scaling lemma has the sign of a logarithm reversed, but the verified repairs below establish the conclusions without changing their hypotheses.
Digit-frequency winning and losing regions
Pages 4–5 and 13–16 · Theorem 2.2 and its proof · arXiv:2401.00614v3
For irrational , density of the logarithmic orbit lets a player rescale a game interval to any prescribed length window, after correcting the sign in Lemma 3.5. The subsequent block strategies force arbitrarily long biased binary blocks for the losing assertions and give Alice a uniform supply of the required digits for the winning assertions. The quantitative inequalities in the theorem are exactly those needed by those strategies, so the central frequency conclusions follow after the auxiliary repair.
The base- fixed-constant badly approximable set is losing in the stated region
Page 7 and pages 16–17 · Theorem 2.5 and its proof · arXiv:2401.00614v3
Put , , , and . The theorem's hypothesis is . At a trigger time with , Bob can center the next ball at a rational ; the lower inequality permits that center and the upper inequality, together with the center-control estimate, traps all later play in the corresponding forbidden interval. Such trigger times exist for every : an irrational logarithmic step gives a dense orbit, while for a rational step Bob chooses the freely available initial logarithmic phase in the projected interval . This supplies the case omitted from the printed proof and verifies the stated theorem.
The binary fixed-constant badly approximable set is winning in the stated region
Page 7 and pages 17–20 · Theorem 2.6 and its proof · arXiv:2401.00614v3
At each relevant dyadic scale, Alice either keeps the current interval away from the unique forbidden neighborhood or advances to the next scale while preserving the inductive distance bound. The theorem's two parameter inequalities make both alternatives legal. The finite number of smaller scales is immaterial because the target is defined by eventual avoidance. Correcting the two local index and exponent typos identified below makes the invariant agree with the displayed strategy and proves the statement.
02Proofs4 reported findingsContains incorrect or incomplete proofs
Two material steps are not correct as written. Lemma 3.5 asks for a positive fractional part below a negative number, and the proof of Theorem 2.5 uses equidistribution despite allowing rational logarithmic game parameters. Both steps have verified repairs. The other discrepancies are uniquely determined notation errors and do not affect the paper's overall correctness.
The logarithmic rescaling inequality has a reversed sign
Pages 9–10 · Lemma 3.5 and proof · arXiv:2401.00614v3
Because , the printed quantity is negative, so the required inequality for a positive fractional part is impossible. Set , , and . Density of the orbit of modulo one gives with . Taking then gives which is the exact rescaling conclusion used later.
The rational logarithmic-step case is omitted
Pages 16–17 · proof of Theorem 2.5 · arXiv:2401.00614v3
The proof invokes equidistribution of the sequence of logarithmic interval lengths, but the theorem does not assume irrational. The repair is to use the freedom in Bob's initial interval length. If the logarithmic step is irrational, the printed density argument applies. If it is rational, Bob chooses the initial phase in the nonempty projected interval modulo one. The phase then returns periodically, producing infinitely many scales with . The same center choice and trapping argument finish the proof. The printed closed-limsup-to-open-limsup inclusion is also reversed; the direct trapping argument proves open membership and needs no such inclusion.
A dyadic distance and one induction index are mistyped
Page 19 · proof of Theorem 2.6 · arXiv:2401.00614v3
When Bob's interval avoids the forbidden neighborhood at scale , the directly obtained distance is , not . In the next induction transition, the new error variable is rather than . The surrounding inequalities use the corrected stronger distance and the next index, so these are uniquely repairable typographical errors.
Several local symbols have unique contextual corrections
Pages 4 and 9–16 · theorem displays and symmetry lemmas · arXiv:2401.00614v3
The statement of Theorem 2.2 omits the backslash in one occurrence of ; the invariant in Lemma 3.3 should read ; and a symmetry sentence reverses membership when passing between and . Each intended symbol is fixed by the adjacent definition and none changes a parameter range or a strategic step.
03Novelty0 reported findingsNo non-novelty findings
No non-novelty findings.