TY - JOUR
T1 - Metastability cascades and prewetting in the SOS model
AU - Gheissari, Reza
AU - Lubetzky, Eyal
N1 - Publisher Copyright:
© The Author(s), under exclusive licence to Springer-Verlag GmbH Germany, part of Springer Nature 2024.
PY - 2025/4
Y1 - 2025/4
N2 - We study Glauber dynamics for the low temperature (2+1)D Solid-On-Solid model on a box of side-length n with a floor at height 0 (inducing entropic repulsion) and a competing bulk external field λ pointing down (the prewetting problem). In 1996, Cesi and Martinelli showed that if the inverse-temperature β is large enough, then along a decreasing sequence of critical points (λc(k))k=0Kβ the dynamics is torpid: its inverse spectral gap is O(1) when λ∈(λc(k+1),λc(k)) whereas it is exp[Θ(n)] at each λc(k) for each k≤Kβ, due to a coexistence of rigid phases at heights k+1 and k. Our focus is understanding (a) the onset of metastability as λn↑λc(k); and (b) the effect of an unbounded number of layers, as we remove the restriction k≤Kβ, and even allow for λn→0 towards the λ=0 case which has O(logn) layers and was studied by Caputo et al. (Ann Probab 42(4):1516-1589, 2014). We show that for any k, possibly growing with n, the inverse gap is exp[Θ~(1/|λn-λc(k)|)] as λ↑λc(k) up to distance n-1+o(1) from this critical point, due to a metastable layer at height k on the way to forming the desired layer at height k+1. By taking λn=n-α (corresponding to kn≍logn), this also interpolates down to the behavior of the dynamics when λ=0. We complement this by extending the fast mixing to all λ uniformly bounded away from (λc(k))k=0∞. Together, these results provide a sharp understanding of the predicted infinite sequence of dynamical phase transitions governed by the layering phenomenon.
AB - We study Glauber dynamics for the low temperature (2+1)D Solid-On-Solid model on a box of side-length n with a floor at height 0 (inducing entropic repulsion) and a competing bulk external field λ pointing down (the prewetting problem). In 1996, Cesi and Martinelli showed that if the inverse-temperature β is large enough, then along a decreasing sequence of critical points (λc(k))k=0Kβ the dynamics is torpid: its inverse spectral gap is O(1) when λ∈(λc(k+1),λc(k)) whereas it is exp[Θ(n)] at each λc(k) for each k≤Kβ, due to a coexistence of rigid phases at heights k+1 and k. Our focus is understanding (a) the onset of metastability as λn↑λc(k); and (b) the effect of an unbounded number of layers, as we remove the restriction k≤Kβ, and even allow for λn→0 towards the λ=0 case which has O(logn) layers and was studied by Caputo et al. (Ann Probab 42(4):1516-1589, 2014). We show that for any k, possibly growing with n, the inverse gap is exp[Θ~(1/|λn-λc(k)|)] as λ↑λc(k) up to distance n-1+o(1) from this critical point, due to a metastable layer at height k on the way to forming the desired layer at height k+1. By taking λn=n-α (corresponding to kn≍logn), this also interpolates down to the behavior of the dynamics when λ=0. We complement this by extending the fast mixing to all λ uniformly bounded away from (λc(k))k=0∞. Together, these results provide a sharp understanding of the predicted infinite sequence of dynamical phase transitions governed by the layering phenomenon.
KW - Glauber dynamics
KW - Metastability
KW - Mixing time
KW - Prewetting
KW - Solid-on-solid model
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U2 - 10.1007/s00440-024-01328-7
DO - 10.1007/s00440-024-01328-7
M3 - Article
AN - SCOPUS:105003744417
SN - 0178-8051
VL - 191
SP - 1485
EP - 1556
JO - Probability Theory and Related Fields
JF - Probability Theory and Related Fields
IS - 3
ER -