Abstract

We adapt the theory of Ruelle-Pollicott resonances to annealed random dynamical systems generated by independent and identically distributed families of maps. Introducing annealed transfer and Koopman operators, we define resonances as elements of the point spectrum of the associated operators and establish a decorrelation formula relating these resonances to the asymptotic decay of annealed correlations. We then study several classes of systems for which the theory can be made explicit. First, we consider a family of piecewise expanding Markov maps of the interval, we construct Banach spaces adapted to the dynamics and obtain a complete description of the annealed resonance spectrum. Then we investigate an inverse spectral problem, proving realisability results for prescribed collections of complex numbers as resonances of suitably constructed annealed dynamical systems.

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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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Detailed mathematical audit

Generated August 18, 2026
01Statements3 reported findingsContains wrong statements

The Blaschke-product spectrum and the full-resonance conclusion for the interval families are correct. The general Jordan expansion is false when its index is identified with geometric multiplicity, and the claimed mixing corollary is false under transitivity alone.

Theorems A and 11Correct

The annealed Blaschke spectrum is correct

Pages 8 and 24–27 · Theorems A and 11 · arXiv:2608.05649v1

The common Hilbert basis makes the averaged Koopman operator compact and triangular. Its nonzero diagonal entries are 11, (ω)ndP(ω)\int(-\omega)^n\,d\mathbb P(\omega), and (ω)ndP(ω)\int(-\overline\omega)^n\,d\mathbb P(\omega). Compactness excludes any further nonzero spectrum, and the row structure gives the stated algebraic and geometric multiplicities after the proof repair recorded below. The deterministic matrix formula used before averaging agrees with the cited analytic-Anosov calculation.

Slipantschuk–Bandtlow–Just, Complete spectral data for analytic Anosov maps of the torus
Proposition 2.2(2) and Lemma A.2Incorrect

Geometric multiplicity does not determine the polynomial powers in a Jordan expansion

Pages 8–9 and 30–32 · Proposition 2.2(2), Lemma A.2 and equations (54)–(64) · arXiv:2608.05649v1

The statements set mim_i equal to geometric multiplicity and truncate the terms nkλinn^k\lambda_i^n at k<mik<m_i. Take the constant Banach scale Wr=C2W_r=\mathbb C^2 and L=(λ10λ),0<λ<1.L=\begin{pmatrix}\lambda&1\\0&\lambda\end{pmatrix},\qquad 0<|\lambda|<1. All compactness, spectral-gap, inclusion, density, and generalized-eigenspace hypotheses hold, but the geometric multiplicity is one while Ln=(λnnλn10λn).L^n=\begin{pmatrix}\lambda^n&n\lambda^{n-1}\\0&\lambda^n\end{pmatrix}. The required nλn1n\lambda^{n-1} contribution is absent from the printed formula. Replace geometric multiplicity by the maximal Jordan-block size, or sum separately over the blocks; with that correction, the intended decorrelation expansion is valid.

Theorem B, Theorem 5, and Corollary 7Incorrect mixing conclusion; resonance conclusion correct

Transitivity does not imply mixing

Pages 9, 12, and 20–21 · Theorem B, Theorem 5 and Corollary 7 · arXiv:2608.05649v1

Use a deterministic one-point base and the four Markov intervals Ij=((j1)/4,j/4)I_j=((j-1)/4,j/4). Define TT with slope 22 so that each of I1,I2I_1,I_2 maps onto (1/2,1)(1/2,1) and each of I3,I4I_3,I_4 maps onto (0,1/2)(0,1/2). This is a transitive piecewise-linear expanding Markov map satisfying every displayed hypothesis, but its irreducible transition matrix has period two. Lebesgue measure is invariant and h=1(0,1/2)1(1/2,1)h=\mathbf1_{(0,1/2)}-\mathbf1_{(1/2,1)} satisfies hT=hh\circ T=-h, so h(hTn)=(1)n\int h(h\circ T^n)=(-1)^n and the system is not mixing. Equivalently, the transfer operator has eigenvalue 1-1. The full decorrelation formula remains correct because that peripheral resonance can be included; only the asserted mixing and spectral-gap consequence fails.

02Proofs5 reported findingsContains incorrect or incomplete proofs

The proofs contain a false Perron–Frobenius inference, an incorrect Jordan-multiplicity argument, and an unproved orthogonality step in the averaged abstract decomposition. The core compactness and interval quasi-compactness arguments are otherwise repairable.

Corollary 7Incorrect as written; no repair at the stated scope

Irreducibility is incorrectly strengthened to primitivity

Pages 20–21 · proof of Corollary 7 · arXiv:2608.05649v1

Perron–Frobenius gives simplicity of the eigenvalue 11 for an irreducible stochastic matrix, but it does not put every other eigenvalue strictly inside the unit circle. An irreducible matrix of period q>1q>1 has peripheral qqth roots of unity. The explicit period-two map in the Statements finding realizes exactly this obstruction. A repair requires an aperiodicity or primitivity hypothesis; it cannot be obtained from the stated transitivity assumption.

Lemma A.2Incorrect as written; verified repair

The Jordan calculation uses the wrong multiplicity

Pages 30–31 · proof of Lemma A.2 · equations (55)–(59) · arXiv:2608.05649v1

A nilpotent part does not satisfy Qimi=0Q_i^{m_i}=0 when mim_i is merely the geometric multiplicity. Its nilpotency order is the largest Jordan-block size. Replacing mim_i by that order and expanding (λiI+Ni)n=k=0si1(nk)λinkNik(\lambda_i I+N_i)^n=\sum_{k=0}^{s_i-1}\binom nk\lambda_i^{n-k}N_i^k gives the required finite polynomial-exponential expansion. This repair propagates through Proposition 2.2 and Theorem 5 without changing the existence of full resonances.

Proof of Theorem 11Incorrect as written; verified repair

The displayed basis vectors are not eigenvectors

Page 27 · proof of Theorem 11 · arXiv:2608.05649v1

The proof says that e(0,k)e_{(0,k)} is an eigenvector, but equation (34) gives Uωe(0,k)=z2k((z1ω)/(1ωz1))kU_\omega e_{(0,k)}=z_2^k((z_1-\omega)/(1-\overline\omega z_1))^k up to normalization, which is not generally a scalar multiple of e(0,k)e_{(0,k)}. The multiplicity conclusion is nevertheless recoverable. Each row carrying a nonzero diagonal value has no off-diagonal entry, so its coordinate functional is an eigenvector of UU^*. For λ0\lambda\ne0, UλIU-\lambda I is Fredholm of index zero; hence dimker(UλI)=dimker(UλI)\dim\ker(U-\lambda I)=\dim\ker(U^*-\overline\lambda I). The triangular finite sections give the algebraic multiplicity as the number of occurrences, so the geometric multiplicity equals it.

Proposition 2.2(1)Incomplete as written; no repair supplied

Orthogonality does not follow by averaging the fibre decompositions

Pages 8 and 31–32 · Proposition 2.2(1) and its proof · arXiv:2608.05649v1

The proof shows only that LL is a compact perturbation of an operator whose norm is bounded by εr(ω)dP(ω)\int\varepsilon_r(\omega)\,d\mathbb P(\omega). It then asserts an orthogonal decomposition L=Πr+NrL=\Pi_r+N_r. Pointwise relations Πω,rNω,r=0\Pi_{\omega,r}N_{\omega,r}=0 do not imply (Πω,r)(Nω,r)=0(\int\Pi_{\omega,r})(\int N_{\omega,r})=0, because cross terms with different ω\omega remain. A spectral projection can give an orthogonal invariant splitting, but the proof does not establish the separately claimed one-step operator-norm bound for its remainder.

Definition 4 and Lemmas 3.2–3.4Typo

Two notation defects have unique harmless corrections

Pages 6–7 and 15–17 · Definition 4 and equations (16), (20) · arXiv:2608.05649v1

In Definition 4, replace the printed remainder o(ε)o(\varepsilon) by o(εn)o(\varepsilon^n). In the Lasota–Yorke displays, the factor λ(k+r1)\lambda^{-(k+r-1)} must multiply hr\lVert h\rVert_r, while the bounded coefficient multiplies hr1\lVert h\rVert_{r-1}. The calculations immediately below the displays derive exactly these corrected inequalities, which are the form needed for the essential-spectral-radius argument.

03Novelty0 reported findingsNo non-novelty findings

No non-novelty findings.

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Paper
arXiv:2608.05649v1
Authors listed
Sakshi Jain, Maxence Phalempin
Audit date
August 18, 2026
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