TY - JOUR
T1 - Macroscopic loops in the loop O(n) model at Nienhuis' critical point
AU - Duminil-Copin, Hugo
AU - Glazman, Alexander
AU - Peled, Ron
AU - Spinka, Yinon
N1 - Publisher Copyright:
© European Mathematical Society 2021
PY - 2021
Y1 - 2021
N2 - The loop O(n) model is a model for a random collection of non-intersecting loops on the hexagonal lattice, which is believed to be in the same universality class as the spin O(n) model. It has been predicted by Nienhuis that for 0 ≤ n ≤ 2, the loop O(n) model exhibits a phase transition at a critical parameter xc(n) = 1/p2 + √2 − n. For 0 < n ≤ 2, the transition line has been further conjectured to separate a regime with short loops when x < xc(n) from a regime with macroscopic loops when x ≥ xc(n). In this paper, we prove that for n ∈ [1, 2] and x = xc(n), the loop O(n) model exhibits macroscopic loops. Apart from the case n = 1, this constitutes the first regime of parameters for which macroscopic loops have been rigorously established. A main tool in the proof is a new positive association (FKG) property shown to hold when n ≥ 1 and 0 < x ≤ 1/√n. This property implies, using techniques recently developed for the random-cluster model, the following dichotomy: either long loops are exponentially unlikely or the origin is surrounded by loops at any scale (box-crossing property). We develop a “domain gluing” technique which allows us to employ Smirnov's parafermionic observable to rule out the first alternative when n ∈ [1, 2] and x = xc(n).
AB - The loop O(n) model is a model for a random collection of non-intersecting loops on the hexagonal lattice, which is believed to be in the same universality class as the spin O(n) model. It has been predicted by Nienhuis that for 0 ≤ n ≤ 2, the loop O(n) model exhibits a phase transition at a critical parameter xc(n) = 1/p2 + √2 − n. For 0 < n ≤ 2, the transition line has been further conjectured to separate a regime with short loops when x < xc(n) from a regime with macroscopic loops when x ≥ xc(n). In this paper, we prove that for n ∈ [1, 2] and x = xc(n), the loop O(n) model exhibits macroscopic loops. Apart from the case n = 1, this constitutes the first regime of parameters for which macroscopic loops have been rigorously established. A main tool in the proof is a new positive association (FKG) property shown to hold when n ≥ 1 and 0 < x ≤ 1/√n. This property implies, using techniques recently developed for the random-cluster model, the following dichotomy: either long loops are exponentially unlikely or the origin is surrounded by loops at any scale (box-crossing property). We develop a “domain gluing” technique which allows us to employ Smirnov's parafermionic observable to rule out the first alternative when n ∈ [1, 2] and x = xc(n).
KW - Conformal invariance
KW - Dichotomy theorem
KW - Dilute Potts model
KW - FKG inequality
KW - Kosterlitz-Thouless phase transition
KW - Loop O(n) model
KW - Macroscopic loops
KW - Parafermionic observable
KW - Russo-Seymour-Welsh theory
KW - Spin representation
KW - Two-dimensional critical phenomena
UR - https://www.scopus.com/pages/publications/85099029948
U2 - 10.4171/JEMS/1012
DO - 10.4171/JEMS/1012
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AN - SCOPUS:85099029948
SN - 1435-9855
VL - 23
SP - 315
EP - 347
JO - Journal of the European Mathematical Society
JF - Journal of the European Mathematical Society
IS - 1
ER -