Abstract

Given a non-atomic standard probability space (Ω,μ)(Ω,μ), we exhibit examples of non-amenable closed topological subgroups of Aut(Ω,μ)\mathrm{Aut}(Ω,μ) whose natural near-action on (Ω,μ)(Ω,μ) is whirly. This answers a 2010 question by Pestov in the negative. The argument proceeds via constructing Gaussian near-actions from topologically faithful unitary representations of non-amenable whirly Polish groups.

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Audited against arXiv v1

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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Generated August 18, 2026
01Statements3 reported findingsCorrect

The faithful ergodic Gaussian realization theorem, the whirliness and inertness results for the three stated families, and the resulting negative answer to Pestov's question are correct. The external structural inputs are used within their hypotheses, and the few notation slips in auxiliary proofs have unique harmless corrections.

Theorem 1.3Correct

Every second-countable unitarily representable group has a faithful ergodic near-action

Pages 2 and 5–7 · Theorem 1.3 and its proof · arXiv:2608.11662v1

A countable family of strong-operator seminorms reduces the faithful representation to a separable invariant Hilbert space. Its finite-dimensional part has compact closure and therefore an ergodic translation action, while the orthogonal complement contains no nonzero finite-dimensional invariant subspace and hence gives a weakly mixing Gaussian near-action. The product representation is still a topological embedding, and the product of an ergodic action with a weakly mixing action is ergodic. This proves all parts of the stated conclusion, including topological faithfulness.

Theorem 1.4Correct

The three families are whirly and inert as claimed

Pages 3 and 20–22 · Theorem 1.4 and its proof · arXiv:2608.11662v1

For L0(μ,G)L^0(\mu,G), each simple function lies in a continuous image of L0(μ,Z)L^0(\mu,\mathbb Z), so the cited whirliness result for non-elliptic diffuse submeasures and extreme amenability for diffuse submeasures propagate by density and quotients. Every unitary in a II1\mathrm{II}_1 factor lies in a diffuse maximal abelian von Neumann subalgebra, whose unitary group is an L0L^0-group. For a full group [E][E], every torsion element lies in a continuous image of L0([0,1],λ;Z)L^0([0,1],\lambda;\mathbb Z) and torsion is dense; the alternative hyperfinite-subrelation argument independently reaches the same conclusion. These deductions match the persistence lemmas proved in Sections 4–5.

Schneider–Solecki, groups without unitary representations
Corollary 1.5Correct

The non-amenable closed whirly subgroup exists

Pages 3 and 22 · Corollary 1.5 and its proof · arXiv:2608.11662v1

Each displayed choice of GG is Polish, unitarily representable, whirly, and non-amenable by the cited L0L^0, von Neumann algebra, or full-group characterization. Theorem 1.3 embeds GG into Aut(Ω,μ)\operatorname{Aut}(\Omega',\mu') with ergodic image. Ergodicity and infinitude rule out a finite atomic probability space, a standard-space isomorphism transports the action to the prescribed non-atomic space, and Raikov completeness makes the embedded image closed. Proposition 4.3 then converts group whirliness into whirliness of the induced ergodic near-action.

02Proofs5 reported findingsCorrect

The central proofs are correct and complete. The Gaussian decomposition, permanence properties, L0L^0 factorization, maximal-abelian-subalgebra reduction, and full-group density argument close all substantive obligations. Three local notation slips have unique corrections and do not change any argument or conclusion.

Proof of Theorem 1.3Correct and complete

The compact and weakly mixing components are handled completely

Pages 5–7 · proof of Theorem 1.3 · arXiv:2608.11662v1

The closure of the finite-dimensional component is compact because its restriction map embeds it into a product of compact orthogonal groups and the closure is Raikov complete. Haar translation supplies the compact ergodic factor. Any finite-dimensional invariant subspace of the complementary representation would belong simultaneously to the finite-dimensional span and its orthogonal complement, so that representation is weakly mixing. The Gaussian Koopman construction is faithful and continuous, and the two factors jointly retain the original representation's topology.

Sections 4–7Correct and complete

The persistence and example arguments are complete

Pages 8–22 · Lemmas 4.2–6.12 and proof of Theorem 1.4 · arXiv:2608.11662v1

Whirliness and inertness are correctly shown to pass through dense subgroups, continuous quotients, and the generated dense union of suitable subgroups. Lemma 6.12 constructs a 11-Lipschitz homomorphism from step functions, then extends it to the Raikov completion; this places every torsion element of [E][E] in a whirly inert subgroup. The cited equivalences for amenability of L0L^0-groups and hyperfinite full groups, together with the standard amenability characterization of unitary groups of von Neumann algebras, are invoked with the required diffuseness, non-atomicity, separability, or factor hypotheses.

Le Maître, Theorem 8.4
Lemma 4.4(b)Typo

The invariant measure is assigned to the wrong group before extension

Page 9 · proof of Lemma 4.4(b), reverse implication · arXiv:2608.11662v1

The proof begins with an action of the dense subgroup HH and prints that μ\mu is 'GG-invariant' before the action has been extended to GG. It must say 'HH-invariant.' The following paragraph then proves exactly that this HH-invariant measure is GG-invariant after extension, so the intended correction is unique and the argument is unchanged.

Lemma 6.7Typo

Dominated convergence uses the original measure

Page 16 · proof of Lemma 6.7 · arXiv:2608.11662v1

In the displayed pairing χBn,f\langle\chi_{B_n},f\rangle, both integrals are printed with dμd\mu. They must use dνd\nu, because the pairing is between L(Ω,B,ν)L^\infty(\Omega,\mathcal B,\nu) and its predual L1(Ω,B,ν)L^1(\Omega,\mathcal B,\nu), while countable additivity of the newly defined μ(B)=τM(ι(χB))\mu(B)=\tau_M(\iota(\chi_B)) is precisely what this convergence proves. Replacing dμd\mu by dνd\nu twice makes the dominated-convergence step valid and leaves the remainder unchanged.

Remark 6.8Typo

The domain symbol changes from XX to Ω\Omega

Page 16 · Remark 6.8 · arXiv:2608.11662v1

The remark starts with a finite measure space (X,B,μ)(X,\mathcal B,\mu) but writes L0(Ω,B,μ;T)L^0(\Omega,\mathcal B,\mu;\mathbb T) in the displayed equality. The unique consistent correction is L0(X,B,μ;T)L^0(X,\mathcal B,\mu;\mathbb T). This notation mismatch has no downstream effect.

03Novelty0 reported findingsNo non-novelty findings

No non-novelty findings.

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Paper
arXiv:2608.11662v1
Authors listed
Yannik Höll, Friedrich Martin Schneider
Audit date
August 18, 2026
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