arXiv:2608.09702v1
Abstract
Let be a topological dynamical system and be its induced system. For a non-empty compact subset , we define as the set of Borel probability measures supported on . In this paper, we systematically study the relationship between various entropies of and of . We show that: where , , and denote the upper capacity topological entropy, the packing topological entropy, and the Bowen topological entropy of , respectively. Additionally, we present a counterexample involving a non-invariant set, demonstrating that the converse of the third assertion is not valid in general.
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Detailed mathematical audit
01Statements4 reported findingsCorrect
For nonempty compact , the upper-capacity and packing entropy equivalences, the Bowen-entropy amplification, and the compact counterexample to the Bowen converse are correct. Theorem 1.3 omits compactness from its first displayed hypothesis; this is a local scope correction consistent with the abstract and the proof and does not lower the substantive status.
Upper-capacity entropy has the zero-or-infinite amplification dichotomy
Pages 2 and 6–9 · Theorem 1.1 and Section 3 · arXiv:2608.09702v1
Weighted atomic embeddings of into multiply upper-capacity entropy by at least , giving infinity whenever has positive entropy. Conversely, an exponentially large separated family of supported measures is discretized by a Bowen-spanning partition of and sent into a finite-dimensional space. The cited Glasner–Weiss combinatorial lemma forces that partition to have exponentially many atoms, proving positivity of the entropy of . The contrapositives yield the zero equivalence.
Packing entropy is positive for exactly when it is positive for
Page 3 and pages 9–14 · Theorem 1.2 and Section 4 · arXiv:2608.09702v1
The Dirac embedding preserves pointwise local entropy and gives the forward inequality. For the converse, the compact-set packing variational principle supplies a measure on with positive upper local entropy. Its barycenter has zero upper local entropy if has zero packing entropy; after restricting most of its mass to a compact low-capacity subset, Lemma 4.2 transfers any remaining positive local entropy back to that subset, giving the required contradiction.
Bowen entropy amplification and failure of the converse
Page 3 and pages 14–17 · Theorem 1.3 and Section 5 · arXiv:2608.09702v1
For compact , product measures and the Bowen variational principle give , and the weighted atomic embedding then makes positive entropy on infinite on . In the binary-shift example, the two coordinate sets have alternating zero lower densities, so their union has zero Bowen entropy, while a family of mixtures of two Bernoulli product measures embeds full product alphabets of arbitrary finite size in and gives infinite Bowen entropy.
Compactness should be retained in the first assertion
Page 3 · statement of Theorem 1.3 · arXiv:2608.09702v1
Insert 'compact' in 'If is non-empty.' Proposition 5.1 and its proof invoke the compact-set variational principle, and the abstract, the common setup, and the counterexample all concern compact subsets. No claim for arbitrary noncompact sets is established, while the one-word restriction makes the theorem match every use and leaves all advertised conclusions intact.
02Proofs4 reported findingsContains incorrect or incomplete proofs
The upper-capacity and Bowen arguments are correct and complete. The packing-entropy converse has one concrete support defect: a normalized restriction to a merely Borel set need not have support contained in that set. A verified repair is available by taking a compact subset before restricting, but the printed proof is incomplete as written.
Restriction to a Borel set need not produce a measure supported on that set
Pages 11–13 · proof of Theorem 4.3, definition of · arXiv:2608.09702v1
The paper defines by the condition . Lemma 4.1 produces a Borel set , but the proof then asserts that belongs to . For nonclosed , the support of this restriction can contain boundary points outside , so the pushed-forward measure need not satisfy the support hypothesis of Lemma 4.2. Repair classification: Verified repair. By inner regularity on the compact metric space, replace by a compact subset whose barycenter mass remains above the required threshold. Monotonicity preserves , is supported on , and all total-variation and local-entropy estimates continue with the same argument after an arbitrarily small adjustment of .
Atomic embeddings and the finite-dimensional separation argument
Pages 6–9 · Section 3 · arXiv:2608.09702v1
The binary weights make the ordered atomic representation injective even when coordinates coincide, the map is equivariant, and product separated sets give the lower bound. In the converse direction, uniform continuity of finitely many test functions controls the discretization error, the tail of the metric contributes less than , and the Glasner–Weiss lemma applies with target dimension , forcing exponential growth of the spanning number of .
Product lower bound and binary-shift counterexample
Pages 14–17 · Section 5 · arXiv:2608.09702v1
For the product measure, the lower pointwise local entropy is superadditive under the max product metric, and integrating plus the compact Bowen variational principle yields the factor . In the example, each coordinate set has lower density zero along its alternating endpoint subsequence, which supplies arbitrarily long Bowen covers with subexponential weight. The supported mixture map records every coordinate parameter in the first test function, so an -ball fixes the first symbols of the product parameter and has mass at most ; Lemma 5.2 then gives entropy at least for every .
The local-mass bound is Lemma 5.2
Page 17 · final paragraph of the proof of Theorem 5.3 · arXiv:2608.09702v1
Replace 'Theorem 5.2' by 'Lemma 5.2'. The immediately preceding result with that number is exactly the local Bowen-ball mass criterion applied here, so the correction is unique and harmless.
03Novelty0 reported findingsNo non-novelty findings
No non-novelty findings.