Counterexamples to integer-coefficient criteria for recurrence along functions from a Hardy field
Pith reviewed 2026-05-19 22:48 UTC · model grok-4.3
The pith
Integer-coefficient conditions on Hardy field functions fail to guarantee thick common return-time sets.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
For the pair f1(t)=t^{3/2} and f2(t)=λ t^{3/2}+t where λ is irrational, every F in nabla_Z(f1,f2) satisfies lim |F(t)| in {0,∞}. Nevertheless there exists E subset N of positive density such that R_f1(E) cap R_f2(E) is piecewise syndetic but not thick. Even under the full integer derivative-span condition the common return-time set may be empty. These facts give negative answers to the questions of Bergelson, Moreira, and Richter on whether the integer-coefficient replacement implies thickness or whether recurrence follows from joint intersectivity of the integer polynomials in poly(f1,...,fk). The constructions use elementary Bohr sets.
What carries the argument
Elementary Bohr sets that produce a positive-density subset E whose return-time intersection R_f1(E) cap R_f2(E) is controlled to be piecewise syndetic but not thick, despite the integer linear combinations in nabla_Z(f1,f2) tending to 0 or infinity.
If this is right
- The integer-coefficient derivative-span condition does not suffice to imply thickness of common return sets.
- Joint intersectivity of the integer polynomials in poly(f1,...,fk) does not guarantee the recurrence conclusion of Theorem A.
- Common return-time sets can be empty even when the full integer derivative-span condition holds for the pair of functions.
Where Pith is reading between the lines
- Similar counterexamples may exist for other pairs of functions drawn from the same Hardy field or with different irrational coefficients.
- The obstructions indicate that recurrence criteria must incorporate more structure from the Hardy field than integer coefficients alone.
- These negative results may limit the scope of multiple-recurrence theorems that rely on polynomial or power-law times in ergodic theory.
Load-bearing premise
The constructions assume that elementary Bohr sets can be chosen to simultaneously achieve positive natural density, make the intersection piecewise syndetic but not thick, and satisfy the recurrence relations for the given Hardy field functions without hidden constraints from the field structure.
What would settle it
A concrete elementary Bohr set E of positive density for which the intersection R_f1(E) cap R_f2(E) is either empty or piecewise syndetic but not thick, while every integer linear combination of the functions and their derivatives still tends to 0 or infinity.
read the original abstract
We give negative answers to two questions of Bergelson, Moreira, and Richter concerning recurrence along functions from a Hardy field. For the pair \(f_1(t)=t^{3/2}\) and \(f_2(t)=\lambda t^{3/2}+t\), where \(\lambda\in\mathbb R\setminus\mathbb Q\), singled out in their integer-coefficient derivative-span question, we prove that every \(F\in\nablaz(f_1,f_2)\) satisfies \(\lim_{t\to\infty}|F(t)|\in\{0,\infty\}\). Nevertheless, there is a set \(E\subset\mathbb N\) of positive natural density such that \(R_{f_1}(E)\cap R_{f_2}(E)\) is piecewise syndetic and not thick. Thus the proposed integer-coefficient replacement does not imply thickness. We further show that, even under the same full integer derivative-span condition, the common return-time set may be empty. This stronger obstruction also gives a negative answer to their question asking whether the recurrence conclusion of Theorem A follows from joint intersectivity of the integer polynomials in \(\operatorname{poly}(f_1,\ldots,f_k)\). The constructions use elementary Bohr sets.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript provides counterexamples to two questions of Bergelson, Moreira, and Richter on recurrence along functions from a Hardy field. For the pair f1(t)=t^{3/2} and f2(t)=λ t^{3/2}+t with λ irrational, it proves that every F in nabla_Z(f1,f2) satisfies lim |F(t)| ∈ {0,∞}. Nevertheless, there exists E ⊂ ℕ of positive natural density such that R_{f1}(E) ∩ R_{f2}(E) is piecewise syndetic but not thick. The paper further shows that the common return-time set may be empty even under the full integer derivative-span condition. Both results are obtained via explicit constructions using elementary Bohr sets.
Significance. If the constructions are valid, the paper supplies concrete negative answers that separate the integer-coefficient derivative-span condition from thickness or non-emptiness of return sets. The use of elementary Bohr sets to produce a positive-density E with the required syndeticity properties while respecting the Hardy-field asymptotics is a technical strength that makes the counterexamples falsifiable and explicit. This clarifies the limitations of the proposed replacement criteria in the literature on Hardy-field recurrence.
major comments (2)
- [§4] §4, Construction of E: The argument that an elementary Bohr set can be chosen to have positive natural density, make R_{f1}(E) ∩ R_{f2}(E) piecewise syndetic but not thick, and remain compatible with the asymptotic independence of f1 and f2 must explicitly rule out linear dependence relations over ℤ that the Hardy-field structure might impose on E−E. Without this verification the separation between the lim |F(t)| condition and non-thickness is not yet load-bearing.
- [§5] §5, Emptiness result: The proof that the common return-time set can be empty under the full integer derivative-span condition relies on a specific choice of Bohr neighborhood; it should include a direct check that this choice does not inadvertently force a non-empty intersection via the joint polynomial structure in poly(f1,f2).
minor comments (2)
- [Introduction] The definition of nabla_Z(f1,f2) in the introduction would benefit from a one-sentence reminder of its relation to the integer span of derivatives, for readers coming from the Bergelson–Moreira–Richter paper.
- [§3] A short paragraph recalling the precise definition of elementary Bohr sets (including the role of the frequency set) would improve readability in §3.
Simulated Author's Rebuttal
We thank the referee for the careful reading and constructive major comments. The points raised concern the explicitness of independence verifications in the constructions of Sections 4 and 5. We address each comment below and will revise the manuscript to incorporate the suggested clarifications.
read point-by-point responses
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Referee: [§4] §4, Construction of E: The argument that an elementary Bohr set can be chosen to have positive natural density, make R_{f1}(E) ∩ R_{f2}(E) piecewise syndetic but not thick, and remain compatible with the asymptotic independence of f1 and f2 must explicitly rule out linear dependence relations over ℤ that the Hardy-field structure might impose on E−E. Without this verification the separation between the lim |F(t)| condition and non-thickness is not yet load-bearing.
Authors: We thank the referee for highlighting this point. In the construction of E in §4, the elementary Bohr set is defined via a frequency α chosen to be linearly independent over Q from the leading coefficients of f1 and f2 (specifically, α is taken from a set of full measure avoiding the countable set of forbidden ratios determined by the Hardy-field asymptotics). This choice ensures that no non-trivial relation ∑ n_i (x_i - y_i) = 0 with n_i ∈ ℤ can hold for differences in E−E in a way that would violate the asymptotic independence or force thickness. We will add a brief paragraph (or short lemma) in the revised §4 that explicitly verifies this independence and confirms that the resulting E−E avoids the relevant linear dependencies. This addition will make the separation between the lim |F(t)| condition and non-thickness fully load-bearing. revision: yes
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Referee: [§5] §5, Emptiness result: The proof that the common return-time set can be empty under the full integer derivative-span condition relies on a specific choice of Bohr neighborhood; it should include a direct check that this choice does not inadvertently force a non-empty intersection via the joint polynomial structure in poly(f1,f2).
Authors: We agree that an explicit check strengthens the argument. The Bohr neighborhood in §5 is chosen with frequency vector and radius such that the defining linear forms are Q-linearly independent from all integer polynomials in poly(f1,f2). By the definition of the Hardy-field functions and the syndeticity properties of the resulting set, this independence precludes any forced non-empty intersection. We will insert a direct verification (as a short remark or auxiliary claim) immediately after the construction in the revised §5, confirming that the chosen parameters avoid the joint polynomial relations and that emptiness is preserved. This revision addresses the referee's concern while leaving the main emptiness result unchanged. revision: yes
Circularity Check
Explicit Bohr-set constructions supply independent counterexamples with no reduction to self-defined inputs or self-citations
full rationale
The paper's central results are obtained by direct, explicit constructions of a positive-density set E from elementary Bohr sets such that R_f1(E) ∩ R_f2(E) is piecewise syndetic but not thick (and a second construction where the intersection is empty), while verifying that every F in nabla_Z(f1,f2) satisfies the limit condition. These constructions are presented as self-contained combinatorial objects that simultaneously meet the density, syndeticity, and non-thickness requirements without invoking fitted parameters, self-referential definitions, or load-bearing citations to prior work by the same authors. No equation or step in the described argument reduces by construction to an input that is itself defined in terms of the output; the Hardy-field compatibility is checked directly on the chosen sets rather than assumed via an ansatz or uniqueness theorem. The derivation chain is therefore independent of the paper's own outputs.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption Standard properties of Hardy fields and the definition of nabla_Z(f1,...,fk).
- domain assumption Existence of Bohr sets with positive natural density that are piecewise syndetic but not thick.
Lean theorems connected to this paper
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IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
every F ∈ ∇_Z-span(f1,f2) satisfies lim |F(t)| ∈ {0,∞} ... Rf1(E) ∩ Rf2(E) is piecewise syndetic but not thick
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IndisputableMonolith/Foundation/AlexanderDuality.leanalexander_duality_circle_linking unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
The constructions use elementary Bohr sets
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
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discussion (0)
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