Depinning of discommensurations for tilted Frenkel-Kontorova chains

TL;DR

This paper investigates how tilting affects discommensurations in Frenkel-Kontorova chains, revealing thresholds where these structures persist or transition to sliding states, and connecting these phenomena to invariant circles in twist maps.

Contribution

It establishes the existence and properties of tilt thresholds for discommensurations and links these to invariant circle conditions in the associated twist map.

Findings

Discommensurations persist up to specific tilt thresholds.

Existence of periodically sliding discommensurations between thresholds.

Connection between tilt thresholds and invariant circles in the twist map.

Abstract

For an untilted Frenkel-Kontorova chain and any rational $p/q$, Aubry and Mather proved there are minimising equilibrium states that are left- and right-asymptotic to neighbouring pairs of spatially periodic minimisers of type $(p,q)$. They are known as {\em discommensurations} (or kinks or fronts), {\em advancing }if the right-asymptotic equilibrium is to the right of the left-asymptotic one, {\em retreating} otherwise. Following work of Middleton, Floria \& Mazo and Baesens \& MacKay, there is a threshold tilt $F_d(p/q)\ge 0$ up to which there continue to be periodic equilibria of type $(p,q)$ and above which there is a globally attracting periodically sliding solution in the space of sequences of type $(p,q)$. In this paper, we prove that there are values $F_d(p/q\pm)$ of tilt with $0\le F_d(p/q\pm) \le F_d(p/q)$, generically positive and less than $F_d(p/q)$, up to which there continue to be equilibrium advancing or retreating discommensurations, respectively, and such that for $F_d(p/q\pm) < F < F_d(p/q)$ there are periodically sliding discommensurations, apart perhaps from exceptional cases with both a degenerate type $(p,q)$ equilibrium and a degenerate advancing equilibrium discommensuration. We give examples, however, to show that equilibrium and periodically sliding discommensurations may co-exist, both above and below $F_d(p/q\pm)$, so the case of discommensurations is not as clean as that of periodic configurations. On the way, we prove that $F_d(\omega) \to F_d(p/q\pm)$ as $\omega \searrow p/q$ or $\nearrow p/q$ respectively. Finally, we prove that $F_d(p/q\pm)=0$ is equivalent to the existence of a rotational invariant circle consisting of periodic orbits of type $(p,q)$ and right-going (respectively left-going) separatrices, for the corresponding twist map on the cylinder.