coefficient and F is a force acting on the adatoms ( F is related to the electric current heating the crystal ). In the limit of fast surface diffusion and slow kinetics of atom attachment-detachment at the steps we formulate a model free of the quasi-static approximation in the calculation of the adatom concentration on the terraces. The linear stability analysis of a step train results in an instability condition in the formτ is the dimensionless life-time of an adatom before desorption, f and η are dimensionless electromigration force and the force of step repulsion whereas V and cr V are the velocity of steps in the train and the critical velocity respectively. As seen instability is expected when either the velocity V is larger than cr V ( this instability is related to the "kinetic memory effect" ), or steps. Numerical integration of the equations for the time evolution of the adatom concentrations and the equations of step motion reveals two different step bunching instabilities: 1) step density waves (small bunches which do not manifest any coarsening) induced by the kinetic memory effect and 2) step bunching with coarsening when the dynamics is dominated by the electromigration. The model developed in this paper also provides very instructive illustrations of the Popkov-Krug dynamical phase transition during sublimation and growth of a vicinal crystal surface.
IntroductionIn a recent paper [1] we advanced a new model for the step dynamics during sublimation and growth of a vicinal crystal surface. This model contains the same physics as the classical Burton, Cabrera, Frank (BCF) theory [2,3,4] but the mathematical treatment deviates from the BCF procedure. In contrast to their assumption that the adatom concentrations i n on the terraces reach instantly their steady state for a given step configuration we analyzed the non-steady state problem [1]. This is relatively easy in the limiting case of fast surface diffusion and slow kinetics of atom attachment and detachment at the steps, since the fast diffusion provides for a constant value of the adatom concentration all over a given terrace. We derived equations for the time evolution of the adatom concentration on the terraces and, also, equations for the step motion. In this way we were able to treat accurately the case when the time to reach steady state concentration of adatoms on the terraces is compatible with the time for nonnegligible change of the step configuration. In such a situation a new effect becomes important -the adatom concentration on a given terrace depends not only on the terrace size but on the "past of the terrace" as well. We call this a "kinetic memory effect". This effect provides a ground for a new type of instability of the regular step distribution.Step density compression waves appear at the vicinal surface as shown by both linear stability analysis and numerical integration of the equations for step motion [1]. Here our aim is to see how the "kinetic memory effect" competes with another (well known) destabilizing factor -th...