TY - JOUR
T1 - Contour Methods for Long-Range Ising Models
T2 - Weakening Nearest-Neighbor Interactions and Adding Decaying Fields
AU - Bissacot, Rodrigo
AU - Endo, Eric O.
AU - van Enter, Aernout C. D.
AU - Kimura, Bruno
AU - Ruszel, Wioletta M.
PY - 2018/8
Y1 - 2018/8
N2 - We consider ferromagnetic long- range Ising models which display phase transitions. They are one- dimensional Ising ferromagnets, in which the interaction is given by Jx, y = J(| x - y|) = 1 | x- y| 2- a with a. [ 0, 1), in particular, J(1) = 1. For this class of models, one way in which one can prove the phase transition is via a kind of Peierls contour argument, using the adaptation of the Fr ohlich- Spencer contours for a = 0, proposed by Cassandro, Ferrari, Merola and Presutti. As proved by Fr ohlich and Spencer for a = 0 and conjectured by Cassandro et al for the region they could treat, a. (0, a+) for a+ = log(3)/ log(2) - 1, although in the literature dealing with contour methods for these models it is generally assumed that J(1) 1, we will show that this condition can be removed in the contour analysis. In addition, combining our theorem with a recent result of Littin and Picco we prove the persistence of the contour proof of the phase transition for any a. [ 0, 1). Moreover, we show that when we add a magnetic field decaying to zero, given by hx = h* center dot (1+| x|) -. and. > max{1- a, 1- a *} where a * 0.2714, the transition still persists.
AB - We consider ferromagnetic long- range Ising models which display phase transitions. They are one- dimensional Ising ferromagnets, in which the interaction is given by Jx, y = J(| x - y|) = 1 | x- y| 2- a with a. [ 0, 1), in particular, J(1) = 1. For this class of models, one way in which one can prove the phase transition is via a kind of Peierls contour argument, using the adaptation of the Fr ohlich- Spencer contours for a = 0, proposed by Cassandro, Ferrari, Merola and Presutti. As proved by Fr ohlich and Spencer for a = 0 and conjectured by Cassandro et al for the region they could treat, a. (0, a+) for a+ = log(3)/ log(2) - 1, although in the literature dealing with contour methods for these models it is generally assumed that J(1) 1, we will show that this condition can be removed in the contour analysis. In addition, combining our theorem with a recent result of Littin and Picco we prove the persistence of the contour proof of the phase transition for any a. [ 0, 1). Moreover, we show that when we add a magnetic field decaying to zero, given by hx = h* center dot (1+| x|) -. and. > max{1- a, 1- a *} where a * 0.2714, the transition still persists.
KW - PHASE-TRANSITION
KW - POTTS MODELS
KW - EXTERNAL FIELDS
KW - LATTICE MODELS
KW - FERROMAGNET
KW - TREES
U2 - 10.1007/s00023-018-0693-3
DO - 10.1007/s00023-018-0693-3
M3 - Article
SN - 1424-0637
VL - 19
SP - 2557
EP - 2574
JO - Annales Henri Poincaré
JF - Annales Henri Poincaré
IS - 8
ER -