Statements (14)
| Predicate | Object |
|---|---|
| gptkbp:instanceOf |
gptkb:mathematical_concept
|
| gptkbp:appliesTo |
completely integrable Hamiltonian systems
|
| gptkbp:describes |
integrable systems
|
| gptkbp:field |
gptkb:Hamiltonian_mechanics
symplectic geometry |
| https://www.w3.org/2000/01/rdf-schema#label |
Arnold–Liouville theorem
|
| gptkbp:implies |
existence of invariant tori in phase space
|
| gptkbp:namedAfter |
gptkb:Joseph_Liouville
gptkb:Vladimir_Arnold |
| gptkbp:publishedIn |
gptkb:Annals_of_Mathematics
|
| gptkbp:state |
integrable Hamiltonian systems can be solved by action-angle coordinates
|
| gptkbp:bfsParent |
gptkb:Vladimir_Arnold
gptkb:V.I._Arnold |
| gptkbp:bfsLayer |
6
|