Metastability for expanding bubbles on a sticky substrate

TL;DR

This paper analyzes a one-dimensional interface model interacting with a sticky substrate, revealing a phase diagram with localized and delocalized phases, and identifies critical lines for static and dynamic behaviors, including metastability.

Contribution

It provides a comprehensive phase diagram for the interface model, including static and dynamic phase transitions, and characterizes metastable behavior and mixing times.

Findings

Identifies the phase boundary between localized and delocalized phases.

Determines the critical line separating polynomial and exponential mixing times.

Provides sharp estimates of mixing times and evidence of metastability.

Abstract

We study the dynamical behavior of a one dimensional interface interacting with a sticky unpenetrable substrate or wall. The interface is subject to two effects going in opposite directions. Contact between the interface and the substrate are given an energetic bonus while an external force with constant intensity pulls the interface away from the wall. Our interface is modeled by the graph of a one-dimensional nearest-neighbor path on $\mathbb{Z}_+$, starting at $0$ and ending at $0$ after $2N$ steps, the wall corresponding to level-zero the horizontal axis. At equilibrium each path $\xi=(\xi_x)_{x=0}^{2N}$, is given a probability proportional to $\lambda^{H(\xi)} \exp(\frac{\sigma}{N}A(\xi))$, where $H(\xi):=\#\{x \ : \xi_x=0\}$ and $A(\xi)$ is the area enclosed between the path $\xi$ and the $x$-axis. We then consider the classical heat-bath dynamics which equilibrates the value of each $\xi_x$ at a constant rate via corner-flip. Investigating the statics of the model, we derive the full phase diagram in $\lambda$ and $\sigma$ of this model, and identify the critical line which separates a localized phase where the pinning force sticks the interface to the wall and a delocalized one, for which the external force stabilizes $\xi$ around a deterministic shape at a macroscopic distance of the wall. On the dynamical side, we identify a second critical line, which separates a rapidly mixing phase (for which the system mixes in polynomial time) to a slow phase where the mixing time grows exponentially. In this slowly mixing regime we obtain a sharp estimate of the mixing time on the $\log$ scale, and provide evidences of a metastable behavior.