A general mechanism of instability in Hamiltonian systems: skipping along a normally hyperbolic invariant manifold
DOI10.3934/dcds.2020166zbMath1454.37054OpenAlexW3011927555MaRDI QIDQ2211125
Rafael de la Llave, Marian Gidea, Teresa M. Seara
Publication date: 12 November 2020
Published in: Discrete and Continuous Dynamical Systems (Search for Journal in Brave)
Full work available at URL: https://doi.org/10.3934/dcds.2020166
instabilityArnold diffusionshadowingscattering mapnormally hyperbolic manifoldscorrectly aligned windows
Stability for nonlinear problems in mechanics (70K20) Bifurcations and instability for nonlinear problems in mechanics (70K50) Stability problems for finite-dimensional Hamiltonian and Lagrangian systems (37J25) Stability problems for problems in Hamiltonian and Lagrangian mechanics (70H14) General theory of finite-dimensional Hamiltonian and Lagrangian systems, Hamiltonian and Lagrangian structures, symmetries, invariants (37J06) Relations of finite-dimensional Hamiltonian and Lagrangian systems with topology, geometry and differential geometry (symplectic geometry, Poisson geometry, etc.) (37J39)
Related Items (3)
Cites Work
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Unnamed Item
- Instability of high dimensional Hamiltonian systems: multiple resonances do not impede diffusion
- Arnold diffusion in arbitrary degrees of freedom and normally hyperbolic invariant cylinders
- Perturbations of geodesic flows by recurrent dynamics
- Arnold diffusion. I: Announcement of results
- A functional analysis approach to Arnold diffusion
- Arnold diffusion in Hamiltonian systems: a priori unstable case
- A numerical study of the topology of normally hyperbolic invariant manifolds supporting Arnold diffusion in quasi-integrable systems
- Kolmogorov theorem revisited
- Unbounded energy growth in Hamiltonian systems with a slowly varying parameter
- Approximately invariant manifolds and global dynamics of spike states
- Drift in phase space: A new variational mechanism with optimal diffusion time
- Global Melnikov theory in Hamiltonian systems with general time-dependent perturbations
- Invariant manifolds and the parameterization method in coupled energy harvesting piezoelectric oscillators
- Arnold diffusion for a complete family of perturbations
- Lectures on partial hyperbolicity and stable ergodicity
- A geometric approach to the existence of orbits with unbounded energy in generic periodic perturbations by a potential of generic geodesic flows of \(\mathbb{T}^2\)
- Arnold's mechanism of diffusion in the spatial circular restricted three-body problem: A semi-analytical argument
- Arnold diffusion in a priori chaotic symplectic maps
- Arnold diffusion of charged particles in ABC magnetic fields
- Geometric properties of the scattering map of a normally hyperbolic invariant manifold
- Orbits of unbounded energy in quasi-periodic perturbations of geodesic flows.
- Über Systeme von linearen partiellen Differentialgleichungen erster Ordnung
- Arnold diffusion far from strong resonances in multidimensionala prioriunstable Hamiltonian systems
- Arnold diffusion in the planar elliptic restricted three-body problem: mechanism and numerical verification
- Transition tori in the planar restricted elliptic three-body problem
- Arnold diffusion for smooth convex systems of two and a half degrees of freedom
- Geography of resonances and Arnold diffusion ina prioriunstable Hamiltonian systems
- Symbolic dynamics of almost collision orbits and skew products of symplectic maps
- Diffusion speed in the Mather problem
- Differentiable conjugacy near compact invariant manifolds
- Existence and persistence of invariant manifolds for semiflows in Banach space
- Evolution of slow variables ina prioriunstable Hamiltonian systems
- Trajectories in a neighbourhood of asymptotic surfaces ofa prioriunstable Hamiltonian systems
- A General Mechanism of Diffusion in Hamiltonian Systems: Qualitative Results
- Arnold Diffusion by Variational Methods
- On Non-Linear Differential Equations of the Second Order: I. the Equation y¨ − k (1-y 2 )y˙ + y = b λk cos(λl + α), k Large
- Invariant manifolds
- Arnold diffusion for a complete family of perturbations with two independent harmonics
This page was built for publication: A general mechanism of instability in Hamiltonian systems: skipping along a normally hyperbolic invariant manifold