arXiv:2607.27932v2

Freidlin-Wentzell collision-laws between self-stabilizing diffusions

Jean-François Jabir, Julian Tugaut

math.PR60H1060J6060K3537A50

Abstract

The present work investigates the asymptotic behaviours at the zero-noise limit of the first near collision-time and first near collision-location between a pair of independent dd-dimensional Brownian-driven self-stabilizing (McKean-Vlasov type) diffusions. These asymptotic are considered in a peculiar setting where the systems evolve in a bi-stable landscape and collisions are only triggered by the combined action of the Brownian noises. As the Brownian perturbations fade away, we show that the near collision-time increases at an explicit exponential rate and that related collision-locations persist in specific regions of the space. These results are mainly derived by tailoring classical Freidlin-Wentzell's exit-time (and exit-location) estimates into collision estimates. Similar asymptotic are established for related mean-field interacting particle system approximation, and for the one-dimensional case (where true collisions can be examined

AI-generated audit

Audit summary

Audited against arXiv v2

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.

Current report

Detailed mathematical audit

Generated August 18, 2026
01Statements2 reported findingsContains unsupported statements

No counterexample to either principal collision law was established. Both remain unverified under the printed assumptions, however. The proof applies the paper's bounded-domain, globally-Lipschitz Freidlin--Wentzell theorem to unbounded domains and polynomial drifts, and its exponentially long coupling uses a local quadratic stability property that does not follow from asymptotic stability. The particle theorem also requires a population threshold depending on the collision radius, while its statement quantifies over one fixed sufficiently large population before taking the radius to zero.

Theorem 1.5Not able to verify

Collision law for the two self-stabilizing diffusions

Pages 9 and 13–28 · Theorem 1.5 and Sections 2–3 · arXiv:2607.27932v2

The action H0H_0 is the natural candidate for the iterated small-radius and small-noise collision cost, and the finite-cover argument would transfer fixed-center hitting laws to the first collision. Two indispensable inputs are not established under Assumptions (A), though. First, Lemma 2.2 invokes Theorem 1.4 outside the theorem's printed bounded-domain and globally-Lipschitz hypotheses. Second, Proposition 3.2 assumes local quadratic attraction of U-U at each well, whereas (A)-(ii) gives only Lyapunov asymptotic stability. Since these inputs control the process for times of order exp(2H/σ2)\exp(2H/\sigma^2), the displayed double limit and persistence conclusion are not verified by the present proof. This is not a claim that the theorem is false.

Theorem 1.6Not able to verify

Collision law for a fixed sufficiently large particle population

Pages 10 and 29–35 · Theorem 1.6 and Section 4 · arXiv:2607.27932v2

This theorem inherits the unresolved Freidlin--Wentzell and local-stability inputs from Theorem 1.5. It also states the iterated limit for every fixed NN above one unspecified threshold. Proposition 4.2 instead produces Nε,κN_{\varepsilon,\kappa} depending on the collision radius and coupling tolerance; the transfer to a radius-ε\varepsilon hitting event requires the tolerance to be smaller than ε\varepsilon. No uniform bound on Nε,κN_{\varepsilon,\kappa} as ε0\varepsilon\downarrow0 is proved. The argument therefore verifies, at most, a formulation in which NN is chosen after fixing ε\varepsilon, not the printed quantifier order.

02Proofs6 reported findingsContains incorrect or incomplete proofs

The finite-cover reductions and many coupling estimates are internally consistent after local notation corrections, but three central obligations remain: extending the exit theorem to the unbounded polynomial-drift setting actually used, justifying exponentially long localization from the stated stability assumption, and making the particle-rank choice uniform in the outer radius limit. The printed definition of the positive small-radius threshold also uses an infimum where its own explanation requires a supremal interval.

Lemma 2.2 and Lemma 2.4Incomplete as written

The recalled exit theorem is applied outside two explicit hypotheses

Pages 8 and 13–17 · Theorem 1.4 and Lemmas 2.2–2.4 · arXiv:2607.27932v2

Theorem 1.4 in the paper assumes an open bounded exit domain and globally Lipschitz drift and diffusion. Lemma 2.2 applies it to G=(Dλ,ε1×Dλ,ε2)cG=(D^1_{\lambda,\varepsilon}\times D^2_{\lambda,\varepsilon})^c and its modified versions. These domains are generally unbounded; for the one-dimensional contractive drift Ψi(x)=(xλi)-\Psi_i(x)=-(x-\lambda_i), each complement (Dλ,εi)c(D^i_{\lambda,\varepsilon})^c is already an unbounded half-line when the target ball misses λi\lambda_i. Moreover, the main drifts Wλi=U+F(λi)W_{\lambda_i}=U+F(\,·-\lambda_i) have the polynomial growth allowed by (A)-(i) and (A)-(iii), not global Lipschitz continuity. No extension theorem or truncation-and-outer-boundary argument is supplied. Downstream dependency: Lemma 2.4, Propositions 2.5, 3.3–3.4, and both main theorems. A repair must prove an unbounded-domain exit law under the paper's coercive polynomial hypotheses or truncate the domains and show uniformly that every artificial outer boundary has strictly larger action.

Proposition 3.2, Step 4Incomplete as written

Asymptotic stability is used as if it implied quadratic local coercivity

Pages 26–27 · Step 4 of Proposition 3.2 · arXiv:2607.27932v2

The proof asserts that the Jacobian of U-U at λ1\lambda_1 is negative definite and hence that, for some ρ,r>0\rho,r>0, B(λ1;r)B(\lambda_1;r) lies in Sρ={x:(xλ1)U(x)ρxλ12}.S_\rho=\{x:(x-\lambda_1)\cdot U(x)\geq\rho\lVert x-\lambda_1\rVert^2\}. Assumption (A)-(ii) states only Lyapunov asymptotic stability. That does not imply hyperbolicity or this quadratic bound: the scalar flow x˙=x3\dot x=-x^3 is asymptotically stable at zero but satisfies xU(x)=x4xU(x)=x^4, which cannot dominate ρx2\rho x^2 near zero. The other assumptions do not add the asserted property for UU itself. This bound is then used to keep EXtλ12\mathbb E\lVert X_t-\lambda_1\rVert^2 small up to exponentially large times. A verified sufficient repair is to assume explicitly that (xλi)U(x)ρixλi2(x-\lambda_i)\cdot U(x)\geq\rho_i\lVert x-\lambda_i\rVert^2 in a neighborhood of each well, or replace Step 4 by a localization argument valid for nonhyperbolic stable equilibria.

Theorem 1.6 and Proposition 4.2Incomplete as written

The population threshold is not uniform in the radius limit

Pages 10 and 29–35 · Theorem 1.6, Proposition 4.2, and Section 4.2 · arXiv:2607.27932v2

Theorem 1.6 first fixes a sufficiently large NN and then takes ε0\varepsilon\downarrow0. Proposition 4.2 chooses Nε,κN_{\varepsilon,\kappa} after ε\varepsilon and κ\kappa, and the bracketing of radius-ε\varepsilon hitting times requires κ<ε\kappa<\varepsilon. The proof gives no bound on sup0<ε<εNε,κ(ε)\sup_{0<\varepsilon<\varepsilon_*}N_{\varepsilon,\kappa(\varepsilon)}. Repair classification: unresolved under the printed theorem. Either establish such a uniform bound, or change the conclusion to state the fixed-ε\varepsilon law with NN(ε)N\geq N(\varepsilon) and specify a joint order of limits.

Equations defining $\varepsilon_c$Typo

An infimum cannot define the advertised largest small-radius interval

Pages 17 and 27 · definitions preceding Propositions 2.5 and 3.4 · arXiv:2607.27932v2

Both definitions print εc\varepsilon_c as the infimum of radii at which the desired strict comparison holds, then call it the largest radius and use the comparison for every 0<ε<εc0<\varepsilon<\varepsilon_c. If the comparison holds for all sufficiently small radii, the printed infimum is zero. The definition dictated by the following prose is εc=sup{r>0:the comparison holds for every ε(0,r)}.\varepsilon_c=\sup\{r>0:\text{the comparison holds for every }\varepsilon\in(0,r)\}. This symbol-level correction does not change the intended results, but the proof must still verify that this set contains a positive interval.

Assumptions and coupling notationTypo

Four local symbols conflict with their immediately stated meaning

Pages 5, 22, and 24 · (A)-(i), (A)-(ii), and Proposition 3.2 · arXiv:2607.27932v2

The strong-convexity inequality in (A)-(i) is printed with \leq although the subsequent deductions require ξU(x)ξCξ2\xi\cdot\nabla U(x)\xi\geq C\lVert\xi\rVert^2; (A)-(ii) writes B(λ1;ε)B(\lambda_1;\varepsilon) for both wells instead of B(λi;ε)B(\lambda_i;\varepsilon). In Proposition 3.2, Sκ(1)S_\kappa^{(1)} and the force estimate use EXTκλ12\mathbb E\lVert X_{T_\kappa}-\lambda_1\rVert^2 where their dependence on the running time and every later line require EXtλ12\mathbb E\lVert X_t-\lambda_1\rVert^2. These replacements are uniquely determined by the surrounding logic and are treated as typos, not adverse statement findings.

Proposition 4.2, Step 5.2.3Incorrect as written

A product probability is used despite interacting particles

Page 33 · Step 5.2.3 of Proposition 4.2 · arXiv:2607.27932v2

The proof bounds the probability that at least cNcN tagged couplings fail by a binomial sum involving ν(σ)\nu(\sigma)^\ell. The failure events are not independent because the Xi,NX^{i,N} interact through their empirical measure, so the product power is unjustified. Repair classification: verified repair. Exchangeability and Markov's inequality give P ⁣(1Ni=1N1Aic)E[N1i1Ai]c=P(A1)c0,\mathbb P\!\left(\frac1N\sum_{i=1}^N\mathbf1_{A_i}\geq c\right)\leq\frac{\mathbb E[N^{-1}\sum_i\mathbf1_{A_i}]}{c}=\frac{\mathbb P(A_1)}{c}\longrightarrow0, which supplies exactly the high-probability conclusion needed in the following step.

03Novelty0 reported findingsNo non-novelty findings

No non-novelty findings.

Detailed audit reportFull reasoning, manuscript locations, and references.
Open report PDF ↗

Author response

Challenge an audit finding

Local workflow preview

A listed author may submit formal evidence that an audit is inaccurate. The response would be considered in a fresh AI re-evaluation; it would not edit the audit automatically.

Paper
arXiv:2607.27932v2
Authors listed
Jean-François Jabir, Julian Tugaut
Audit date
August 18, 2026
  1. 01Establish identityMatch an authenticated scholarly identity to this paper.
  2. 02Submit evidenceIdentify the finding and give a formal mathematical response.
  3. 03Re-evaluateA separate agent checks the response and records a disposition.
Recommended production method

Authenticate with ORCID, then require an exact arXiv match

MathAudit should accept the identity only when ORCID OAuth authenticates the claimant's iD and this exact arXiv paper appears in arXiv's public authority feed for that iD. A matching name alone is not sufficient.

ORCID OAuth and arXiv authority-record lookup are not connected in this local prototype.

Email fallback for papers without a linked ORCID

A production fallback could send a one-time link only when the submitted address matches an independently maintained author-contact allowlist for this paper. MathAudit must return the same message for every address so the form cannot reveal which contacts are on that list.

This demonstration does not send, store, or compare the address.

Structured response preview

This form remains unavailable until production identity verification succeeds. Nothing entered here is submitted.

This panel never establishes authorship in the local prototype. A production result should be described narrowly as an authenticated ORCID match or control of a separately allowlisted author-contact mailbox.