The Hammersley–Clifford theorem is a result in probability theory, mathematical statistics and statistical mechanics that gives necessary and sufficient conditions under which a strictly positive probability distribution (of events in a probability space) can be represented as events generated by a Markov network (also known as a Markov random field). It is the fundamental theorem of random fields. It states that a probability distribution that has a strictly positive mass or density satisfies one of the Markov properties with respect to an undirected graph G if and only if it is a Gibbs random field, that is, its density can be factorized over the cliques (or complete subgraphs) of the graph.
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| - Teoremo de Hammersley–Clifford (eo)
- Hammersley–Clifford theorem (en)
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| - La Teoremo de Hammersley–Clifford temas pri probabloteorio, statistiko kaj statistika mekaniko. Ĝi difinas la necesan kaj sufiĉan kondiĉojn tial, kial probabla distribuo povas reprezentiĝi kiel Markova reto. Ĝi estas la fundamenta teoremo pri hazarda kampo. La teoremo asertas, ke probablo distribuo, kiu havas strikte pozitivan mason aŭ denson, estas Markova al sendirekta grafeo G, se kaj nur se ĝi estas Gibsa. Tio estas, ĝia denso eblas faktoriĝi laŭ la klikoj de la grafeo. (eo)
- The Hammersley–Clifford theorem is a result in probability theory, mathematical statistics and statistical mechanics that gives necessary and sufficient conditions under which a strictly positive probability distribution (of events in a probability space) can be represented as events generated by a Markov network (also known as a Markov random field). It is the fundamental theorem of random fields. It states that a probability distribution that has a strictly positive mass or density satisfies one of the Markov properties with respect to an undirected graph G if and only if it is a Gibbs random field, that is, its density can be factorized over the cliques (or complete subgraphs) of the graph. (en)
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| - This is completely underspecified!! A probability distribution *on what*? Without specifying the graph, lattice, state, process, or other underlying structure where the "randomness" is occuring, the definition makes little sense. (en)
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| - La Teoremo de Hammersley–Clifford temas pri probabloteorio, statistiko kaj statistika mekaniko. Ĝi difinas la necesan kaj sufiĉan kondiĉojn tial, kial probabla distribuo povas reprezentiĝi kiel Markova reto. Ĝi estas la fundamenta teoremo pri hazarda kampo. La teoremo asertas, ke probablo distribuo, kiu havas strikte pozitivan mason aŭ denson, estas Markova al sendirekta grafeo G, se kaj nur se ĝi estas Gibsa. Tio estas, ĝia denso eblas faktoriĝi laŭ la klikoj de la grafeo. La rilaton inter Markova kaj Gibsa reto unue studis Roland Dobrushin kaj Frank Spitzer sub kunteksto de statistika mekaniko. La teoremo nomiĝas memore al John Hammersley kaj Peter Clifford, kiuj pruvis la ekvivalenton en nepublikigita raporto en 1971. Pli simpla pruvo per inkluziveco-ekskluda principo donis sendepende , Preston kaj Sherman en 1973, kun posta pruvo fare de en 1974. (eo)
- The Hammersley–Clifford theorem is a result in probability theory, mathematical statistics and statistical mechanics that gives necessary and sufficient conditions under which a strictly positive probability distribution (of events in a probability space) can be represented as events generated by a Markov network (also known as a Markov random field). It is the fundamental theorem of random fields. It states that a probability distribution that has a strictly positive mass or density satisfies one of the Markov properties with respect to an undirected graph G if and only if it is a Gibbs random field, that is, its density can be factorized over the cliques (or complete subgraphs) of the graph. The relationship between Markov and Gibbs random fields was initiated by Roland Dobrushin and Frank Spitzer in the context of statistical mechanics. The theorem is named after John Hammersley and , who proved the equivalence in an unpublished paper in 1971. Simpler proofs using the inclusion–exclusion principle were given independently by Geoffrey Grimmett, Preston and Sherman in 1973, with a further proof by Julian Besag in 1974. (en)
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