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The Planar Ising Model and Total Positivity

dc.creatorLis, Marcin
dc.date.accessioned2016-12-02
dc.date.accessioned2018-11-24T23:27:02Z
dc.date.available2017-03-02T11:26:43Z
dc.date.available2018-11-24T23:27:02Z
dc.date.issued2017-01-01
dc.identifierhttps://www.repository.cam.ac.uk/handle/1810/262826
dc.identifier.urihttp://repository.aust.edu.ng/xmlui/handle/123456789/3935
dc.description.abstractA matrix is called totally positive (resp. totally nonnegative) if all its minors are positive (resp. nonnegative). Consider the Ising model with free boundary conditions and no external field on a planar graph G. Let $a_1$,..., $a_k$ , $b_k$ ,..., $b_1$ be vertices placed in a counterclockwise order on the outer face of $G$. We show that the $k$ $\times$ $k$ matrix of the two-point spin correlation functions $M_{i,j}$ = $\langle$$\sigma$$_{a_{i}}$$\sigma$$_{b_{j}}$$\rangle$ is totally nonnegative. Moreover, det $M$ > 0 if and only if there exist $k$ pairwise vertex-disjoint paths that connect $a_i$ with $b_i$ . We also compute the scaling limit at criticality of the probability that there are $k$ parallel and disjoint connections between $a_i$ and $b_i$ in the double random current model. Our results are based on a new distributional relation between double random currents and random alternating flows of Talaska [37].
dc.languageen
dc.publisherSpringer
dc.publisherJournal of Statistical Physics
dc.rightshttp://creativecommons.org/licenses/by/4.0/
dc.rightshttp://creativecommons.org/licenses/by/4.0/
dc.rightshttp://creativecommons.org/licenses/by/4.0/
dc.rightsAttribution 4.0 International
dc.rightsAttribution 4.0 International
dc.rightsAttribution 4.0 International
dc.subjectIsing model
dc.subjecttotal positivity
dc.subjectrandom currents
dc.subjectalternating flows
dc.titleThe Planar Ising Model and Total Positivity
dc.typeArticle


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