KINETIC SURFACE ROUGHENING .2. HYPERCUBE-STACKING MODELS

被引:106
作者
TANG, LH
FORREST, BM
WOLF, DE
机构
[1] FORSCHUNGSZENTRUM JULICH, FORSCHUNGSZENTRUM, INST FESTKORPERFORSCH, W-5170 JULICH 1, GERMANY
[2] RUHR UNIV BOCHUM, FAK PHYS & ASTRON, W-4630 BOCHUM, GERMANY
[3] UNIV HEIDELBERG, INST THEORET PHYS, W-6900 HEIDELBERG, GERMANY
来源
PHYSICAL REVIEW A | 1992年 / 45卷 / 10期
关键词
D O I
10.1103/PhysRevA.45.7162
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
The roughening behavior of a moving surface under a deposition and evaporation dynamics is explored within the hypercube-stacking model. One limiting case of the model is an equilibrium surface, which exhibits thermal roughening for surface dimension d less-than-or-equal-to 2. Another limiting case is nonequilibrium irreversible growth, where the model is shown to map exactly to zero-temperature directed polymers on a hypercubic lattice with a random energy distribution. Results of exact calculations for d = 1 and of large-scale Monte Carlo simulations [N = 2(20), 11520(2), and 2 x 192(3) surface sites for d = 1, 2, and 3, respectively] are presented that establish the Kardar-Parisi-Zhang equation as the correct continuum description of the growth process. For pure deposition (i.e., irreversible growth), careful analysis of surface width data yields the exponents beta(2) = 0.240 +/- 0.001 and beta(3) = 0.180 +/- 0.005, which violate a number of recent conjectures. By allowing for evaporation, we observe a less rapid increase of the surface roughness as a function of time. This phenomenon is consistently explained by a crossover scenario for d = 1 and 2 but a nonequilibrium roughening transition for d = 3, as predicted by a perturbative renormalization-group analysis of the Kardar-Parisi-Zhang equation. Detailed predictions on crossover scaling from the renormalization-group analysis are also confirmed by simulation data. In the d = 1 case, some of the continuum parameters characterizing the renormalization-group flow are obtained explicitly in terms of the lattice parameters via the exact calculation of steady-state properties of the model.
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页码:7162 / 7179
页数:18
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