Kolmogorov–Arnold–Moser theory
E320432
Kolmogorov–Arnold–Moser theory is a fundamental result in dynamical systems that explains the persistence of quasi-periodic motions in nearly integrable Hamiltonian systems under small perturbations.
All labels observed (3)
| Label | Occurrences |
|---|---|
| KAM theory | 2 |
| Kolmogorov–Arnold–Moser theory canonical | 2 |
| Kolmogorov’s invariant torus theorem | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T3037537 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.
Target entity: Kolmogorov–Arnold–Moser theory Context triple: [Andrei Kolmogorov, notableWork, Kolmogorov–Arnold–Moser theory]
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A.
Poincaré–Birkhoff fixed-point theorem
The Poincaré–Birkhoff fixed-point theorem is a fundamental result in dynamical systems and topology that guarantees the existence of at least two fixed points for certain area-preserving twist maps of an annulus.
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B.
Kovalevskaya top
The Kovalevskaya top is a famous integrable case of the motion of a rigid body about a fixed point in classical mechanics, discovered and analyzed by mathematician Sofia Kovalevskaya.
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C.
Carathéodory–Jacobi–Lie theorem
The Carathéodory–Jacobi–Lie theorem is a fundamental result in symplectic geometry and Hamiltonian mechanics that provides canonical local coordinates adapted to a given set of commuting functions.
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D.
Jacobi integral
The Jacobi integral is a conserved quantity in celestial mechanics and dynamical systems that simplifies the analysis of motion in rotating reference frames, particularly in the restricted three-body problem.
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E.
Poincaré recurrence theorem
The Poincaré recurrence theorem is a fundamental result in dynamical systems and ergodic theory stating that certain systems will, after a sufficiently long but finite time, return arbitrarily close to their initial state.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Kolmogorov–Arnold–Moser theory Target entity description: Kolmogorov–Arnold–Moser theory is a fundamental result in dynamical systems that explains the persistence of quasi-periodic motions in nearly integrable Hamiltonian systems under small perturbations.
-
A.
Poincaré–Birkhoff fixed-point theorem
The Poincaré–Birkhoff fixed-point theorem is a fundamental result in dynamical systems and topology that guarantees the existence of at least two fixed points for certain area-preserving twist maps of an annulus.
-
B.
Kovalevskaya top
The Kovalevskaya top is a famous integrable case of the motion of a rigid body about a fixed point in classical mechanics, discovered and analyzed by mathematician Sofia Kovalevskaya.
-
C.
Carathéodory–Jacobi–Lie theorem
The Carathéodory–Jacobi–Lie theorem is a fundamental result in symplectic geometry and Hamiltonian mechanics that provides canonical local coordinates adapted to a given set of commuting functions.
-
D.
Jacobi integral
The Jacobi integral is a conserved quantity in celestial mechanics and dynamical systems that simplifies the analysis of motion in rotating reference frames, particularly in the restricted three-body problem.
-
E.
Poincaré recurrence theorem
The Poincaré recurrence theorem is a fundamental result in dynamical systems and ergodic theory stating that certain systems will, after a sufficiently long but finite time, return arbitrarily close to their initial state.
- F. None of above. chosen
Statements (48)
| Predicate | Object |
|---|---|
| instanceOf |
mathematical theory
ⓘ
result in dynamical systems ⓘ theorem in Hamiltonian dynamics ⓘ |
| abbreviation |
Kolmogorov–Arnold–Moser theory
self-linksurface differs
ⓘ
surface form:
KAM theory
|
| appliesTo |
area-preserving maps
ⓘ
nearly integrable Hamiltonian systems ⓘ small perturbations of integrable systems ⓘ symplectic diffeomorphisms ⓘ |
| assumes | non-degeneracy conditions on the integrable Hamiltonian ⓘ |
| characterizedBy |
control of small divisors via Diophantine conditions
ⓘ
use of iterative schemes to construct invariant tori ⓘ |
| describes |
persistence of invariant tori
ⓘ
persistence of quasi-periodic motions ⓘ |
| explains |
stability of quasi-periodic orbits under small perturbations
ⓘ
survival of invariant tori of positive measure ⓘ |
| field |
Hamiltonian mechanics
ⓘ
dynamical systems ⓘ mathematical physics ⓘ symplectic geometry ⓘ |
| hasConsequence |
existence of KAM tori in phase space
ⓘ
long-term stability of planetary motions in celestial mechanics ⓘ |
| historicalDevelopment |
extended by Vladimir Arnold in the 1960s
ⓘ
initiated by Andrey Kolmogorov in the 1950s ⓘ refined by Jürgen Moser in the 1960s ⓘ |
| implies |
coexistence of regular and chaotic motion
ⓘ
existence of invariant tori of positive Lebesgue measure ⓘ persistence of most invariant tori under sufficiently small perturbations ⓘ |
| influenced |
development of symplectic topology
ⓘ
modern theory of Hamiltonian chaos ⓘ |
| namedAfter |
Andrei Kolmogorov
ⓘ
surface form:
Andrey Kolmogorov
Jürgen Moser ⓘ Vladimir Arnold ⓘ |
| relatedTo |
Arnold diffusion
ⓘ
Kolmogorov–Arnold–Moser theory self-linksurface differs ⓘ
surface form:
Kolmogorov’s invariant torus theorem
Nekhoroshev theory ⓘ standard map ⓘ twist maps ⓘ |
| studiedIn |
accelerator physics
ⓘ
celestial mechanics ⓘ nonlinear oscillations ⓘ plasma physics ⓘ |
| usesConcept |
Diophantine conditions
ⓘ
analytic Hamiltonians ⓘ canonical transformations ⓘ non-resonance conditions ⓘ perturbation theory ⓘ small divisor problems ⓘ symplectic maps ⓘ |
How these facts were elicited
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Subject: Kolmogorov–Arnold–Moser theory Description of subject: Kolmogorov–Arnold–Moser theory is a fundamental result in dynamical systems that explains the persistence of quasi-periodic motions in nearly integrable Hamiltonian systems under small perturbations.
Referenced by (5)
Full triples — surface form annotated when it differs from this entity's canonical label.