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- Arnold_diffusion abstract "In applied mathematics, Arnold diffusion is the phenomenon of instability of integrable Hamiltonian systems. The phenomenon is named after Vladimir Arnold who was the first to publish a result in the field in 1964. More precisely, Arnold diffusion refers to results asserting the existence of solutions to nearly integrable Hamiltonian systems that exhibit a significant change in the action variables.".
- Arnold_diffusion wikiPageID "23813473".
- Arnold_diffusion wikiPageRevisionID "563633889".
- Arnold_diffusion hasPhotoCollection Arnold_diffusion.
- Arnold_diffusion subject Category:Dynamical_systems.
- Arnold_diffusion type Abstraction100002137.
- Arnold_diffusion type Attribute100024264.
- Arnold_diffusion type DynamicalSystem106246361.
- Arnold_diffusion type DynamicalSystems.
- Arnold_diffusion type PhaseSpace100029114.
- Arnold_diffusion type Space100028651.
- Arnold_diffusion comment "In applied mathematics, Arnold diffusion is the phenomenon of instability of integrable Hamiltonian systems. The phenomenon is named after Vladimir Arnold who was the first to publish a result in the field in 1964. More precisely, Arnold diffusion refers to results asserting the existence of solutions to nearly integrable Hamiltonian systems that exhibit a significant change in the action variables.".
- Arnold_diffusion label "Arnold diffusion".
- Arnold_diffusion sameAs m.06_vrqc.
- Arnold_diffusion sameAs Q4795328.
- Arnold_diffusion sameAs Q4795328.
- Arnold_diffusion sameAs Arnold_diffusion.
- Arnold_diffusion wasDerivedFrom Arnold_diffusion?oldid=563633889.
- Arnold_diffusion isPrimaryTopicOf Arnold_diffusion.