首页> 外文期刊>The European physical journal, B. Condensed matter physics >Scaling and universality in models of step bunching: the “C+–C-” model
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Scaling and universality in models of step bunching: the “C+–C-” model

机译:步束模型的缩放和通用性:“ C + –C-”模型

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We recently introduced a novel model of step flow crystal growth – the so-called “C+–C-” model [B. Ranguelov et al., C.R. Acad. Bulgare Sci. 60, 389 (2007)]. In this paper we aim to develop a complete picture of the model’s behaviour in the framework of the notion of universality classes. The basic assumption of the model is that the reference (“equilibrium”) densities used to compute the supersaturation might be different on either side of a step, so CL/CR = 1 (L/R stands for left/right in a step train descending from left to right), and that this will eventually cause destabilization of the regular step train. Linear stability analysis considering perturbation of the whole step train shows that the vicinal is always unstable when the condition CL/CR > 1 is fulfilled. Numerical integration of the equations of step motion combined with an original monitoring scheme(s) results in obtaining the exact size- and time- scaling of the step bunches in the limit of long times (including the numerical prefactors). Over a broad range of parameters the surface morphology is characterized by the appearance of the minimal interstep distance at the beginning of the bunches (at the trailing edge of the bunch) and may be described by a single universality class, different from those already generated by continuum theories [A. Pimpinelli et al., Phys. Rev. Lett. 88, 206103 (2002), J. Krug et al., Phys. Rev. B 71, 045412 (2005)]. In particular, the scaling of the minimal interstep distance lmin in the new universality class is shown to be lmin = (Sn/N)1/(n+1), where N is the number of steps in the bunch, n is the exponent in the step-step repulsion law U 1/dn0 for two steps placed a distance d0 apart and Sn is a combination of the model parameters. It is also shown that N scales with time with universal exponent 1/2 independent of n. For the regime of slow diffusion it is obtained for the first time that the time scaling depends only on the destabilization parameter CL/CR. The bunching outside the parameter region where the above scaling exists cannot be assigned to a specific universality class and thus should be considered non-universal.
机译:我们最近介绍了一种新型的逐步流动晶体生长模型,即所谓的“ C + –C-”模型[B。 Ranguelov等,C.R。Acad。保加利亚科学。 60,389(2007)]。在本文中,我们旨在在通用性类的概念框架中完整地描述模型的行为。该模型的基本假设是,用于计算过饱和度的参考(“平衡”)密度在台阶的任一侧可能会有所不同,因此CL / CR = 1(L / R代表台阶中的左/右)从左到右下降),最终将导致常规脚踏车不稳定。考虑整个步幅扰动的线性稳定性分析表明,满足条件CL / CR> 1时,邻域总是不稳定的。步进运动方程的数值积分与原始的监测方案结合在一起,可以在很长时间内(包括数字前置因子)获得台阶束的精确尺寸和时间标度。在广泛的参数范围内,表面形态的特征是在束的开始处(束的后沿)出现最小步距,并且可以用单个通用性类来描述,这不同于已经由连续论[A. Pimpinelli et al。,Phys。牧师88,206103(2002),J.Krug等人,Phys。 B 71,045412(2005)。特别是,新通用性类别中最小步距间距离lmin的标度显示为lmin =(Sn / N)1 /(n + 1),其中N是束中的步数,n是指数在阶跃推斥定律U 1 / dn0中,两步之间的距离为d0,Sn是模型参数的组合。还表明,N随时间缩放,通用指数为1/2,与n无关。对于慢扩散状态,首次获得时间标度仅取决于去稳定化参数CL / CR的信息。存在上述缩放比例的参数区域之外的束不能分配给特定的通用性类,因此应视为非通用性。

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