2203.07350
Cпектры cамоподобных эргодических действий
V. V. Ryzhikov
correctmedium confidence
- Category
- math.DS
- Journal tier
- Specialist/Solid
- Processed
- Sep 28, 2025, 12:56 AM
- arXiv Links
- Abstract ↗PDF ↗
Audit review
The paper states and proves two claims: (i) for any M⊂N there exists a Poisson suspension with spectral multiplicity set M∪{∞} (Theorem 1), and (ii) there exists a Gaussian flow St such that the time-maps Sp^n have multiplicities {1,∞} for n≤0 and {p^n,∞} for n>0, and an associated infinite tensor-power flow Tt whose T_{p^n} are pairwise non-isomorphic for n≤0 and pairwise isomorphic for n>0 (Theorem 2). Both claims, together with the key functorial identity that G(T) and P(T) are spectrally isomorphic to exp(T)=⊕_{n≥0}T^{⊙n}, are explicitly stated and used in the note (see the abstract and statements of Theorems 1 and 2, and the exp-functor identity in the introduction: G(T),P(T)≅exp(T) ). The proof of Theorem 1 builds specific self-similar rank-one transformations T_m of type (p_m,8) and shows that exp(⊕_{m∈M} mT_m) has multiplicity set M∪{∞}, with higher chaoses yielding a countable (i.e., infinite) multiplicity and being spectrally disjoint from the first chaos (see the decomposition with Q and the intertwining argument) . Theorem 2 is obtained by constructing an orthogonal flow Ot with the p-self-similar spectral structure so that Op^n has simple spectrum for n≤0 and homogeneous multiplicity p^n for n>0, and then passing to the Gaussian flow St=exp(Ot); the tensor-power variant Tt is then handled explicitly . By contrast, the model’s “Phase 2” solution contains a fatal error in the flow part: starting from O1≅⊕_{j=0}^{p−1}e^{2πij/p}U, one has Op^n=O1^{p^n}=⊕_{j=0}^{p−1}U^{p^n}, giving at most multiplicity p (not p^n) on the first chaos. The claimed growth to p^n does not follow from that construction. The automorphism/flow claims for negative times are also left unjustified. While the model’s method for Poisson multiplicities M∪{∞} is broadly in the right spirit (via exp-functor and disjoint rotated copies), several steps are under-justified (e.g., ensuring the needed rotated phases via group extensions; ensuring disjointness; and the precise route to ∞ via higher chaoses). Hence the paper’s results and proofs are consistent and correct as presented, whereas the model’s proof, particularly for the flow, is incorrect.
Referee report (LaTeX)
\textbf{Recommendation:} minor revisions \textbf{Journal Tier:} specialist/solid \textbf{Justification:} The manuscript presents clean constructions achieving precise control of spectral multiplicities for Poisson suspensions and Gaussian flows via self-similar rank-one methods. The arguments leverage the exp-functor identity and careful control of tensor-product spectra, leading to M∪{∞} realizations and prime-power multiplicity profiles in flows. While concise, the exposition could be slightly expanded to make some key steps self-contained (e.g., details on the p-self-similar spectral measure and the disjointness argument between the first chaos and higher chaoses). Overall, the results appear correct and will be of interest to specialists in spectral theory of dynamical systems.