DYNAMICS OF (2+1)-DIMENSIONAL SOS SURFACES ABOVE A WALL: SLOW MIXING INDUCED BY ENTROPIC REPULSION'
成果类型:
Article
署名作者:
Caputo, Pietro; Lubetzky, Eyal; Martinelli, Fabio; Sly, Allan; Toninelli, Fabio Lucio
署名单位:
Roma Tre University; Microsoft; University of California System; University of California Berkeley; Centre National de la Recherche Scientifique (CNRS); Centre National de la Recherche Scientifique (CNRS); Ecole Centrale de Lyon; Institut National des Sciences Appliquees de Lyon - INSA Lyon; Universite Claude Bernard Lyon 1; Universite Jean Monnet
刊物名称:
ANNALS OF PROBABILITY
ISSN/ISSBN:
0091-1798
DOI:
10.1214/13-AOP836
发表日期:
2014
页码:
1516-1589
关键词:
kosterlitz-thouless transition
roughening transition
statistical-mechanics
ising-model
interface
tension
droplet
摘要:
We study the Glauber dynamics for the (2 + 1)D Solid-On-Solid model above a hard wall and below a far away ceiling, on an L x L box of Z(2) with zero boundary conditions, at large inverse-temperature P. It was shown by Bricmont, El Mellouki and Frohlich [J. Stat. Phys. 42 (1986) 743-798] that the floor constraint induces an entropic repulsion effect which lifts the surface to an average height H um log L. As an essential step in understanding the effect of entropic repulsion on the Glauber dynamics we determine the equilibrium height H to within an additive constant: H = (1/4 beta) log L + O(1). We then show that starting from zero initial conditions the surface rises to its final height H through a sequence of metastable transitions between consecutive levels. The time for a transition from height h = aH, a is an element of (0, 1), to height h 1 is roughly exp(cL(a)) for some constant c > 0. In particular, the mixing time of the dynamics is exponentially large in L, that is, T-MIX >= e(cL). We also provide the matching upper bound Tivnix <= e(c'L), requiring a challenging analysis of the statistics of height contours at low temperature and new coupling ideas and techniques. Finally, to emphasize the role of entropic repulsion we show that without a floor constraint at height zero the mixing time is no longer exponentially large in L.
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