Chapman–Kolmogorov equation
E254907
The Chapman–Kolmogorov equation is a fundamental relation in the theory of stochastic processes that expresses how transition probabilities of a Markov process over longer time intervals can be obtained by integrating over intermediate states.
All labels observed (2)
| Label | Occurrences |
|---|---|
| Chapman–Kolmogorov equation canonical | 1 |
| Markov property of Brownian motion | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T2325347 — 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: Chapman–Kolmogorov equation Context triple: [Markov process, relatedTo, Chapman–Kolmogorov equation]
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A.
Kolmogorov backward equation
The Kolmogorov backward equation is a fundamental partial differential equation in stochastic processes that characterizes the time evolution of expected values of functionals of Markov processes, complementary to the Fokker–Planck (forward) equation.
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B.
Fokker–Planck equation
The Fokker–Planck equation is a partial differential equation that describes the time evolution of the probability density function of a stochastic (random) process, such as Brownian motion.
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C.
Feynman–Kac formula
The Feynman–Kac formula is a fundamental result connecting solutions of certain partial differential equations with expectations over stochastic processes, forming a bridge between quantum mechanics, probability theory, and mathematical finance.
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D.
Itô’s lemma
Itô’s lemma is a fundamental result in stochastic calculus that generalizes the chain rule to functions of stochastic processes, especially Brownian motion.
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E.
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.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Chapman–Kolmogorov equation Target entity description: The Chapman–Kolmogorov equation is a fundamental relation in the theory of stochastic processes that expresses how transition probabilities of a Markov process over longer time intervals can be obtained by integrating over intermediate states.
-
A.
Kolmogorov backward equation
The Kolmogorov backward equation is a fundamental partial differential equation in stochastic processes that characterizes the time evolution of expected values of functionals of Markov processes, complementary to the Fokker–Planck (forward) equation.
-
B.
Fokker–Planck equation
The Fokker–Planck equation is a partial differential equation that describes the time evolution of the probability density function of a stochastic (random) process, such as Brownian motion.
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C.
Feynman–Kac formula
The Feynman–Kac formula is a fundamental result connecting solutions of certain partial differential equations with expectations over stochastic processes, forming a bridge between quantum mechanics, probability theory, and mathematical finance.
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D.
Itô’s lemma
Itô’s lemma is a fundamental result in stochastic calculus that generalizes the chain rule to functions of stochastic processes, especially Brownian motion.
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E.
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.
- F. None of above. chosen
Statements (48)
| Predicate | Object |
|---|---|
| instanceOf |
mathematical equation
ⓘ
probability theory concept ⓘ stochastic process concept ⓘ |
| appliesTo |
Markov processes
ⓘ
surface form:
Markov chains
Markov diffusion processes ⓘ Markov processes ⓘ continuous-time Markov processes ⓘ discrete-time Markov processes ⓘ |
| assumes |
Markov property of the process
ⓘ
time parameter can be ordered ⓘ |
| category | Markov process theory ⓘ |
| coreIdea | transition probabilities over long intervals can be obtained via intermediate states ⓘ |
| describes | relation between transition probabilities at different times ⓘ |
| discreteTimeForm | P_{ij}(m+n) = \sum_k P_{ik}(m) P_{kj}(n) ⓘ |
| ensures | compatibility of transition probabilities over overlapping time intervals ⓘ |
| equivalentTo | semigroup property P_{s,t} = P_{s,u} P_{u,t} ⓘ |
| expresses |
composition law for transition probabilities
ⓘ
semigroup property of Markov transition operators ⓘ |
| field |
Markov processes
ⓘ
probability theory ⓘ stochastic processes ⓘ |
| formalStatement | P(X_t \in B \mid X_s = x) = \int P(X_t \in B \mid X_u = y) \, P(X_u \in dy \mid X_s = x) for s < u < t ⓘ |
| generalizes | law of total probability for Markov processes ⓘ |
| implies | Markov property over multiple time steps ⓘ |
| involves |
integration over intermediate states for continuous state spaces
ⓘ
summation over intermediate states for discrete state spaces ⓘ |
| mathematicalDomain |
functional analysis
ⓘ
measure-theoretic probability ⓘ |
| namedAfter |
Andrei Kolmogorov
ⓘ
surface form:
Andrey Kolmogorov
Sydney Chapman ⓘ |
| relatedTo |
Fokker–Planck equation
ⓘ
Kolmogorov backward equation ⓘ Fokker–Planck equation ⓘ
surface form:
Kolmogorov forward equation
Markov semigroup ⓘ master equation ⓘ transition probability kernel ⓘ |
| relates | short-time transition probabilities to long-time transition probabilities ⓘ |
| role |
consistency condition for finite-dimensional distributions of Markov processes
ⓘ
fundamental relation for Markov transition functions ⓘ |
| usedFor |
computing multi-step transition probabilities from one-step transitions
ⓘ
constructing Markov processes from transition kernels ⓘ |
| usedIn |
Markov processes
ⓘ
surface form:
Markov chain theory
derivation of Kolmogorov backward equation ⓘ derivation of Kolmogorov forward equation ⓘ financial mathematics ⓘ population dynamics ⓘ queueing theory ⓘ statistical physics ⓘ |
How these facts were elicited
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Subject: Chapman–Kolmogorov equation Description of subject: The Chapman–Kolmogorov equation is a fundamental relation in the theory of stochastic processes that expresses how transition probabilities of a Markov process over longer time intervals can be obtained by integrating over intermediate states.
Referenced by (2)
Full triples — surface form annotated when it differs from this entity's canonical label.