Lyapunov vector
E181626
A Lyapunov vector is a mathematical construct in dynamical systems theory that characterizes the directions in phase space associated with exponential growth or decay rates quantified by Lyapunov exponents.
All labels observed (1)
| Label | Occurrences |
|---|---|
| Lyapunov vector canonical | 2 |
How this entity was disambiguated
This entity first appeared as the object of triple T1597813 — 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: Lyapunov vector Context triple: [Aleksandr Lyapunov, notableWork, Lyapunov vector]
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A.
Onsager–Machlup function
The Onsager–Machlup function is a functional in stochastic process theory that characterizes the most probable paths of fluctuating systems, playing a key role in nonequilibrium statistical mechanics and large deviation theory.
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B.
Lie derivative
The Lie derivative is a fundamental differential operator in differential geometry that measures how a tensor field changes along the flow generated by a vector field.
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C.
Laplace operator
The Laplace operator is a second-order differential operator widely used in mathematics and physics to describe phenomena such as diffusion, heat flow, and wave propagation.
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D.
Ornstein–Uhlenbeck process
The Ornstein–Uhlenbeck process is a continuous-time stochastic process that models mean-reverting random motion, widely used in physics and quantitative finance to describe systems fluctuating around a long-term equilibrium.
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E.
Poynting vector
The Poynting vector is a fundamental quantity in electromagnetism that represents the directional energy flux (power per unit area) carried by an electromagnetic field.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Lyapunov vector Target entity description: A Lyapunov vector is a mathematical construct in dynamical systems theory that characterizes the directions in phase space associated with exponential growth or decay rates quantified by Lyapunov exponents.
-
A.
Onsager–Machlup function
The Onsager–Machlup function is a functional in stochastic process theory that characterizes the most probable paths of fluctuating systems, playing a key role in nonequilibrium statistical mechanics and large deviation theory.
-
B.
Lie derivative
The Lie derivative is a fundamental differential operator in differential geometry that measures how a tensor field changes along the flow generated by a vector field.
-
C.
Laplace operator
The Laplace operator is a second-order differential operator widely used in mathematics and physics to describe phenomena such as diffusion, heat flow, and wave propagation.
-
D.
Ornstein–Uhlenbeck process
The Ornstein–Uhlenbeck process is a continuous-time stochastic process that models mean-reverting random motion, widely used in physics and quantitative finance to describe systems fluctuating around a long-term equilibrium.
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E.
Poynting vector
The Poynting vector is a fundamental quantity in electromagnetism that represents the directional energy flux (power per unit area) carried by an electromagnetic field.
- F. None of above. chosen
Statements (47)
| Predicate | Object |
|---|---|
| instanceOf |
mathematical concept
ⓘ
object in dynamical systems theory ⓘ |
| appliesTo |
continuous-time dynamical systems
ⓘ
discrete-time dynamical systems ⓘ |
| associatedWith |
linearized dynamics
ⓘ
tangent space of a trajectory ⓘ variational equations ⓘ |
| belongsTo | Oseledec splitting ⓘ |
| characterizes |
directions in phase space
ⓘ
directions of exponential decay ⓘ directions of exponential growth ⓘ |
| computedBy |
Benettin algorithm
ⓘ
QR-based methods ⓘ covariant Lyapunov vector algorithms ⓘ |
| correspondsTo | a particular Lyapunov exponent ⓘ |
| definedBy |
Lyapunov exponents
ⓘ
surface form:
Oseledec multiplicative ergodic theorem
|
| dependsOn |
choice of norm up to equivalence class
ⓘ
invariant measure of the system ⓘ |
| differsFrom | eigenvector of instantaneous Jacobian in general nonlinear systems ⓘ |
| forms | a basis adapted to the Lyapunov exponents ⓘ |
| hasProperty |
can be covariant
ⓘ
can be forward-time or backward-time ⓘ defined along a trajectory ⓘ time-dependent ⓘ |
| hasType |
backward Lyapunov vector
ⓘ
covariant Lyapunov vector ⓘ forward Lyapunov vector ⓘ |
| livesIn | tangent space ⓘ |
| namedAfter | Aleksandr Lyapunov ⓘ |
| quantifiedBy | Lyapunov exponents ⓘ |
| relatedTo |
Lyapunov exponents
ⓘ
surface form:
Lyapunov characteristic exponent
Lyapunov exponents ⓘ
surface form:
Lyapunov exponent
Lyapunov exponents ⓘ
surface form:
Lyapunov spectrum
eigenvectors of the Jacobian in linear systems ⓘ |
| studiedIn |
applied mathematics
ⓘ
ergodic theory ⓘ |
| usedFor |
characterizing chaotic attractors
ⓘ
hyperbolicity analysis ⓘ identifying stable directions ⓘ identifying unstable directions ⓘ mode decomposition in high-dimensional systems ⓘ predictability studies ⓘ sensitivity analysis ⓘ |
| usedIn |
chaos theory
ⓘ
dynamical systems ⓘ nonlinear dynamics ⓘ stability analysis ⓘ |
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Subject: Lyapunov vector Description of subject: A Lyapunov vector is a mathematical construct in dynamical systems theory that characterizes the directions in phase space associated with exponential growth or decay rates quantified by Lyapunov exponents.
Referenced by (2)
Full triples — surface form annotated when it differs from this entity's canonical label.