Answers are grounded in this paper and cite their sources.
We study creep dynamics of a two-dimensional interface driven through a periodic potential using dynamic renormalization-group methods. We find that the nature of weak-drive transport depends qualitatively on whether the temperature T is above or below the equilibrium roughening transition temperature Tc. Above Tc, the velocity-force characteristics are Ohmic, with linear mobility exhibiting a jump discontinuity across the transition. For T<~Tc, the transport is highly nonlinear, exhibiting an interesting crossover in temperature and weak external force F. For intermediate drive, F>F*, we find near Tc^- a power-law velocity-force characteristics v(F)~F^σ, with σ-1∝ ̃ \~t, and well below Tc, v(F)~e^-(F*/F)^2 ̃ \~t, with ̃ \~t=(1-T/Tc). In the limit of vanishing drive (FF*), the velocity-force characteristics cross over to v(F)~e^-(F₀/F), and are controlled by soliton nucleation.
No takes yet. Share an insight, caveat, or question.
Ettouhami et al. (2003) studied this question.
Synapse has enriched 10 related papers. Consider them for comparative context: