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The Blume–Emery–Griffiths Model on the FAD Point and on the AD Line

We analyse the Blume–Emery–Griffiths (BEG) model on the lattice Z d on the ferromagnetic-antiquadrupolar-disordered (FAD) point and on the antiquadrupolar-disordered (AD) line. In our analysis on the FAD point, we introduce a Gibbs sampler of the ground states at zero temperature, and we exploit it...

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Bibliographic Details
Published in:Journal of statistical physics 2023-10, Vol.190 (11), Article 170
Main Authors: Lima, Paulo C., Mariani, Riccardo, Procacci, Aldo, Scoppola, Benedetto
Format: Article
Language:English
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Summary:We analyse the Blume–Emery–Griffiths (BEG) model on the lattice Z d on the ferromagnetic-antiquadrupolar-disordered (FAD) point and on the antiquadrupolar-disordered (AD) line. In our analysis on the FAD point, we introduce a Gibbs sampler of the ground states at zero temperature, and we exploit it in two different ways: first, we perform via perfect sampling an empirical evaluation of the spontaneous magnetization at zero temperature, finding a non-zero value in d = 3 and a vanishing value in d = 2 . Second, using a careful coupling with the Bernoulli site percolation model in d = 2 , we prove rigorously that under imposing + boundary conditions, the magnetization in the center of a square box tends to zero in the thermodynamical limit and the two-point correlations decay exponentially. Also, using again a coupling argument, we show that there exists a unique zero-temperature infinite-volume Gibbs measure for the BEG. In our analysis of the AD line we restrict ourselves to d = 2 and, by comparing the BEG model with a Bernoulli site percolation in a matching graph of Z 2 , we get a condition for the vanishing of the infinite-volume limit magnetization improving, for low temperatures, earlier results obtained via expansion techniques.
ISSN:1572-9613
0022-4715
1572-9613
DOI:10.1007/s10955-023-03181-9