TY - JOUR

T1 - Harmonic pinnacles in the Discrete Gaussian model

AU - Lubetzky, Eyal

AU - Martinelli, Fabio

AU - Sly, Allan

N1 - Publisher Copyright:
© 2016, Springer-Verlag Berlin Heidelberg.

PY - 2016/6/1

Y1 - 2016/6/1

N2 - The 2D Discrete Gaussian model gives each height function η:Z2→Z a probability proportional to exp (- βH(η)) , where β is the inverse-temperature and H(η)=∑x∼y(ηx-ηy)2 sums over nearest-neighbor bonds. We consider the model at large fixed β, where it is flat unlike its continuous analog (the Discrete Gaussian Free Field). We first establish that the maximum height in an L× L box with 0 boundary conditions concentrates on two integers M, M + 1 with M∼(1/2πβ)logLloglogL. The key is a large deviation estimate for the height at the origin in Z2, dominated by “harmonic pinnacles”, integer approximations of a harmonic variational problem. Second, in this model conditioned on η≥ 0 (a floor), the average height rises, and in fact the height of almost all sites concentrates on levels H, H + 1 where H∼M/2. This in particular pins down the asymptotics, and corrects the order, in results of Bricmont et al. (J. Stat. Phys. 42(5–6):743–798, 1986), where it was argued that the maximum and the height of the surface above a floor are both of order logL. Finally, our methods extend to other classical surface models (e.g., restricted SOS), featuring connections to p-harmonic analysis and alternating sign matrices.

AB - The 2D Discrete Gaussian model gives each height function η:Z2→Z a probability proportional to exp (- βH(η)) , where β is the inverse-temperature and H(η)=∑x∼y(ηx-ηy)2 sums over nearest-neighbor bonds. We consider the model at large fixed β, where it is flat unlike its continuous analog (the Discrete Gaussian Free Field). We first establish that the maximum height in an L× L box with 0 boundary conditions concentrates on two integers M, M + 1 with M∼(1/2πβ)logLloglogL. The key is a large deviation estimate for the height at the origin in Z2, dominated by “harmonic pinnacles”, integer approximations of a harmonic variational problem. Second, in this model conditioned on η≥ 0 (a floor), the average height rises, and in fact the height of almost all sites concentrates on levels H, H + 1 where H∼M/2. This in particular pins down the asymptotics, and corrects the order, in results of Bricmont et al. (J. Stat. Phys. 42(5–6):743–798, 1986), where it was argued that the maximum and the height of the surface above a floor are both of order logL. Finally, our methods extend to other classical surface models (e.g., restricted SOS), featuring connections to p-harmonic analysis and alternating sign matrices.

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U2 - 10.1007/s00220-016-2628-5

DO - 10.1007/s00220-016-2628-5

M3 - Article

AN - SCOPUS:84969179694

SN - 0010-3616

VL - 344

SP - 673

EP - 717

JO - Communications In Mathematical Physics

JF - Communications In Mathematical Physics

IS - 3

ER -