Abstract:We discuss a Curie-Weiss model with two groups in the critical regime. This is the region where the central limit theorem does not hold any more but the mean magnetization still goes to zero as the number of spins grows. We show that the total magnetization normalized by N 3/4 converges to a non-trivial distribution which is not Gaussian, just as in the single-group Curie-Weiss model.
“…This is stated in [16] for the bipartite model. In [24] the authors prove the existence of such a phase transition using the method of moments. Of course, with that method one cannot obtain an exponential speed of convergence as in Corollary 1.2.…”
Section: Resultsmentioning
confidence: 99%
“…formula (4.1) in [23]. Later, they were rediscovered as interesting models for statistical mechanics systems, see [18], [15], [8], [26], [24], as well as models for social interactions between several groups, e.g. in [17], [1], [28].…”
We study a block spin mean-field Ising model. For the vector of block magnetizations we prove Large Deviation Principles and Central Limit Theorems under general assumptions for the block interaction matrix. Using the exchangeable pair approach of Stein's method we are also able to establish a speed of convergence for the Central Limit Theorem for the vector of block magnetizations in the high temperature regime.
“…This is stated in [16] for the bipartite model. In [24] the authors prove the existence of such a phase transition using the method of moments. Of course, with that method one cannot obtain an exponential speed of convergence as in Corollary 1.2.…”
Section: Resultsmentioning
confidence: 99%
“…formula (4.1) in [23]. Later, they were rediscovered as interesting models for statistical mechanics systems, see [18], [15], [8], [26], [24], as well as models for social interactions between several groups, e.g. in [17], [1], [28].…”
We study a block spin mean-field Ising model. For the vector of block magnetizations we prove Large Deviation Principles and Central Limit Theorems under general assumptions for the block interaction matrix. Using the exchangeable pair approach of Stein's method we are also able to establish a speed of convergence for the Central Limit Theorem for the vector of block magnetizations in the high temperature regime.
“…Note that Z is of order 1 √ N . This either, follows from Theorem 6 and Remark from the paper by Kirsch and Toth [16] cited at the beginning of Section 3 or from Theorem 3.1 directly: As noted in Remark 3.3 1 N 3/4 i σ i converges to a nondegenerate limit distribution. Since Z ≥ |ζ| as a consequence of β ≥ |α| (α = 1, i.e.…”
Section: Proof Of Theorem 13mentioning
confidence: 75%
“…Indeed, in view of Theorem 3.1 below the main tool in this reference does not work, because at least for α > 0, and α + β = 2 the vector √ N (m 1 , m 2 ) is not asymptotically Gaussian. Moreover, considering Theorem 6 and Remark 7 in [16] one may wonder, whether an exact reconstruction of (S, S c ) on the basis of the correlations between the spins is possible at all. There, the authors show that for α > 0 and α+β = 2 asymptotically:…”
Section: A Limit Theoremmentioning
confidence: 99%
“…The first of these papers uses a very general interaction structure, while the latter investigates the situation in the spirit of social interaction models or statistical physics models on random graphs, see [23], [3], [7], and [18]. A related version of this model has been investigated using the method of moments in [15], [17] and [16]. The article by Berthet et al is motivated by a considerable amount of articles investigating block models in the recent past, see e.g.…”
We show how to exactly reconstruct the block structure at the critical line in the so-called Ising block model. This model was recently re-introduced by Berthet, Rigollet and Srivastavaz in [2]. There the authors show how to exactly reconstruct blocks away from the critical line and they give an upper bound on the number of observations one needs. Our technique relies on a combination of their methods with fluctuation results obtained in [20]. The latter are extended to the full critical regime. We find that the number of necessary observations depends on whether the interaction parameter between two blocks is positive or negative: In the first case, there are about N log N observations required to exactly recover the block structure, while in the latter √ N log N observations suffice.
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