Back to search
2111.12377

SLIDING MOTION ON TANGENTIAL SETS OF FILIPPOV SYSTEMS

Tiago Carvalho, Douglas D. Novaes, Durval J. Tonon

correctmedium confidence
Category
Not specified
Journal tier
Strong Field
Processed
Sep 28, 2025, 12:56 AM

Audit review

The candidate’s proof reconstructs the paper’s Theorem 3: after φ-regularization, one can rewrite the dynamics as a singular perturbation problem possessing a slow manifold Stan diffeomorphic to M, and the reduced flow restricted to Stan is conjugate to the tangential sliding vector field Ztan. The paper proves this by straightening (h,η), rescaling x_n/ε, and constructing Stan = {(u,0,w*(u))} (with w*(u)=φ^{-1}(λ*(u,0,0))) and a direct conjugacy, whereas the candidate augments with a fast auxiliary variable λ to render the graph λ=φ(h/ε) invariant and then performs a slow-time reduction; both routes yield the same reduced dynamics under the same hypothesis 〈dηZ+,dηZ−〉=−‖dηZ+‖‖dηZ−‖≠0 on M. The statements and constructions match the paper’s definitions and Theorem 3 and its proof structure (Definition 1–2, Theorem 1, Definition 3, and Section 4) .

Referee report (LaTeX)

\textbf{Recommendation:} minor revisions

\textbf{Journal Tier:} strong field

\textbf{Justification:}

Both the paper and the candidate demonstrate a correct equivalence between the tangential sliding vector field and the reduced flow of a suitably regularized singularly perturbed system near a tangential manifold M. The candidate uses an augmented fast variable λ to enforce invariance of the regularization graph and then reduces; the paper uses coordinate straightening and direct rescaling of x\_n/ε. The conclusions coincide, and assumptions match. Minor clarifications on time reparametrization scope and explicit identification of slow-set conditions would improve clarity.