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- Lee–Yang_theorem abstract "In statistical mechanics, the Lee–Yang theorem states that if partition functions of certain models in statistical field theory with ferromagnetic interactions are considered as functions of an external field, then all zeros are purely imaginary (or on the unit circle after a change of variable). The first version was proved for the Ising model by T. D. Lee and C. N. Yang (1952) (Lee & Yang 1952). Their result was later extended to more general models by several people. Asano in 1970 extended the Lee-Yang theorem to the Heisenberg model and provided a simpler proof using Asano contractions. Simon & Griffiths (1973) extended the Lee–Yang theorem to certain continuous probability distributions by approximating them by a superposition of Ising models. Newman (1974) gave a general theorem stating roughly that the Lee–Yang theorem holds for a ferromagnetic interaction provided it holds for zero interaction. Lieb & Sokal (1981) generalized Newman's result from measures on R to measures on higher-dimensional Euclidean space.There has been some speculation about a relationship between the Lee–Yang theorem and the Riemann hypothesis about the Riemann zeta function; see (Knauf 1999).".
- Lee–Yang_theorem wikiPageExternalLink p404.
- Lee–Yang_theorem wikiPageExternalLink p410.
- Lee–Yang_theorem wikiPageExternalLink 1103859251.
- Lee–Yang_theorem wikiPageExternalLink 1103919874.
- Lee–Yang_theorem wikiPageID "19661214".
- Lee–Yang_theorem wikiPageLength "6952".
- Lee–Yang_theorem wikiPageOutDegree "17".
- Lee–Yang_theorem wikiPageRevisionID "693894192".
- Lee–Yang_theorem wikiPageWikiLink Asano_contraction.
- Lee–Yang_theorem wikiPageWikiLink Cambridge_University_Press.
- Lee–Yang_theorem wikiPageWikiLink Category:Statistical_mechanics_theorems.
- Lee–Yang_theorem wikiPageWikiLink Charles_M._Newman.
- Lee–Yang_theorem wikiPageWikiLink Communications_on_Pure_and_Applied_Mathematics.
- Lee–Yang_theorem wikiPageWikiLink Gaussian_function.
- Lee–Yang_theorem wikiPageWikiLink Heisenberg_model_(quantum).
- Lee–Yang_theorem wikiPageWikiLink Ising_model.
- Lee–Yang_theorem wikiPageWikiLink Measure_(mathematics).
- Lee–Yang_theorem wikiPageWikiLink Partition_function_(statistical_mechanics).
- Lee–Yang_theorem wikiPageWikiLink Physical_Review.
- Lee–Yang_theorem wikiPageWikiLink Riemann_hypothesis.
- Lee–Yang_theorem wikiPageWikiLink Riemann_zeta_function.
- Lee–Yang_theorem wikiPageWikiLink Statistical_field_theory.
- Lee–Yang_theorem wikiPageWikiLink Statistical_mechanics.
- Lee–Yang_theorem wikiPageWikiLinkText "Lee–Yang theorem".
- Lee–Yang_theorem author1Link "T. D. Lee".
- Lee–Yang_theorem author2Link "C. N. Yang".
- Lee–Yang_theorem first "C. N.".
- Lee–Yang_theorem first "T. D.".
- Lee–Yang_theorem last "Lee".
- Lee–Yang_theorem last "Yang".
- Lee–Yang_theorem wikiPageUsesTemplate Template:Citation.
- Lee–Yang_theorem wikiPageUsesTemplate Template:Harv.
- Lee–Yang_theorem wikiPageUsesTemplate Template:Harvs.
- Lee–Yang_theorem wikiPageUsesTemplate Template:Harvtxt.
- Lee–Yang_theorem year "1952".
- Lee–Yang_theorem subject Category:Statistical_mechanics_theorems.
- Lee–Yang_theorem type Mechanic.
- Lee–Yang_theorem type Redirect.
- Lee–Yang_theorem type Theorem.
- Lee–Yang_theorem comment "In statistical mechanics, the Lee–Yang theorem states that if partition functions of certain models in statistical field theory with ferromagnetic interactions are considered as functions of an external field, then all zeros are purely imaginary (or on the unit circle after a change of variable). The first version was proved for the Ising model by T. D. Lee and C. N. Yang (1952) (Lee & Yang 1952). Their result was later extended to more general models by several people.".
- Lee–Yang_theorem label "Lee–Yang theorem".
- Lee–Yang_theorem sameAs Q6516611.
- Lee–Yang_theorem sameAs リー・ヤンの定理.
- Lee–Yang_theorem sameAs m.04mz5ds.
- Lee–Yang_theorem sameAs Q6516611.
- Lee–Yang_theorem wasDerivedFrom Lee–Yang_theorem?oldid=693894192.
- Lee–Yang_theorem isPrimaryTopicOf Lee–Yang_theorem.