1988
DOI: 10.1007/bf01022985
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Discontinuity of the magnetization in one-dimensional 1/�x?y�2 Ising and Potts models

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Cited by 343 publications
(420 citation statements)
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“…where − ê 1 L;β,q is notation for the thermal state obtained with all boundary spins set toê 1 . The upper and lower bounds,…”
Section: Percolation and Magnetizationmentioning
confidence: 99%
See 1 more Smart Citation
“…where − ê 1 L;β,q is notation for the thermal state obtained with all boundary spins set toê 1 . The upper and lower bounds,…”
Section: Percolation and Magnetizationmentioning
confidence: 99%
“…It is now well established [1,4,10,12,23] that the characteristics of one system can be completely expressed in terms of the other. In particular the critical behavior (if any) of the spin-system translates directly into critical geometrical behavior in the corresponding random cluster model.…”
Section: Introductionmentioning
confidence: 99%
“…Indeed, in the Ising (and also Potts) model, a lowtemperature symmetry breaking occurs even in some recurrent dimensions; e.g., in d = 2 for the nearest-neighbor interactions. For what determines the presence and absence of symmetry breaking in d = 1, see the work of Aizenman, Chayes, Chayes and Newman [3] and references therein.…”
Section: Literature Remarksmentioning
confidence: 99%
“…When q ≥ 1, the associated probability measure satisfies the FKG lattice condition (see Refs. 1,12), and therefore satisfies the FKG inequality (which may be stated roughly as 'increasing events are positively correlated'). This useful inequality implies properties of stochastic comparison which are of substantial value in studying any associated phase transition.…”
Section: Introductionmentioning
confidence: 99%
“…1,15). Such measures have a phase transition at a critical value p = p c (q) that marks the onset of an infinite cluster (or connected component) of the graph.…”
Section: Introductionmentioning
confidence: 99%