2201.12190
Characteristic matrix functions for delay differential equations with symmetry
Babette de Wolff
correcthigh confidence
- Category
- Not specified
- Journal tier
- Strong Field
- Processed
- Sep 28, 2025, 12:56 AM
- arXiv Links
- Abstract ↗PDF ↗
Audit review
The paper’s Theorem 2.3 states precisely that Δ(z) = I − z h^{-1}F(Θ(h)p, z) is a characteristic matrix for Uh = h^{-1}U(Θ(h)p, 0), in the sense of Definition 2.2 where analytic E(z), F(z) are invertible for all z and satisfy the block factorization (Δ(z) ⊕ I) = F(z) (I ⊕ (I − zUh)) E(z). The proof proceeds by writing Uh as V + R with V Volterra and R finite rank, applying Theorem 3.5 to obtain Δ, and then identifying C(I − zV)^{-1}D = h^{-1}F(τ, z) (thus Δ(z) = I − z h^{-1}F(τ, z)) . By contrast, the model’s construction incorrectly asserts that I − zUh is invertible for all z (treating Uh as Volterra), which is false since the nonzero spectrum of Uh is precisely what Δ captures. It then defines F(z) with a lower-right block (I − zUh), contradicting the requirement that F(z) be invertible for all z in Definition 2.2 and leading to an inconsistency in the factorization step. Hence the paper is correct, while the model’s argument fails at the core operator-theoretic step.
Referee report (LaTeX)
\textbf{Recommendation:} minor revisions \textbf{Journal Tier:} strong field \textbf{Justification:} The work provides a rigorous and elegant reduction from an infinite-dimensional Floquet-type stability question with symmetry to a finite-dimensional characteristic determinant. The use of a Volterra-plus-finite-rank decomposition, together with characteristic-matrix theory, is sound and well-suited to the problem. The result is timely and relevant for equivariant delayed-feedback control. Some minor clarifications and signposting would further aid readers.