2108.05074
On the Lyapunov instability in Lagrangian dynamics
J. M. Burgos, M. Paternain
correctmedium confidence
- Category
- Not specified
- Journal tier
- Strong Field
- Processed
- Sep 28, 2025, 12:56 AM
- arXiv Links
- Abstract ↗PDF ↗
Audit review
The paper proves Lyapunov instability under the hypotheses dU(∇ρ f)=O(U) and ||ι_{∇ρ f} dµ||=O(U^{1/2}) via a time-rescaling and a gradient-flow–adapted coordinate argument that yields a positive drift of f along solutions and hence exit from any small neighborhood. The candidate solution establishes the same instability using an energy-based differential inequality for h(t)=df_x(v), integrates it twice, and shows exit from thin f-slabs for arbitrarily small initial velocities. The approaches are logically consistent and reach the same conclusion; the model’s derivation has a minor constant slip in bounding the magnetic term but is easily fixed without affecting correctness.
Referee report (LaTeX)
\textbf{Recommendation:} minor revisions
\textbf{Journal Tier:} strong field
\textbf{Justification:}
The paper offers a clear and useful instability criterion for Lagrangian systems with magnetic terms, extending Newtonian results to a broader setting without assuming the magnetic field vanishes at the equilibrium. The proof, based on a well-chosen time-rescaling and coordinates adapted to the gradient flow of f, is careful and rigorous. The result contributes to Palamodov’s program and is of interest to the Hamiltonian/Lagrangian dynamics community. Some minor editorial clarifications would improve readability.