The anisotropic kinetic function, i

The anisotropic kinetic function, i.e., Eq. (6), for different d
values is shown in Fig. 4(a), which indicates a peak value at 451;
the peak value gives b 11 ¼5.1 s/m (n¼10). The larger d value gives
a narrower distribution. The evolution of the interface morphol-
ogies ( f ¼0) based on d ¼4, 16, and 64 are, respectively, shown in
Fig. 4(b), (c) and (d) for n¼10 and e 4 ¼0.25. Small perturbations
(40 small waves) are introduced at the beginning. The interval
for each interface is 0.22 s and the total elapsed time is 3.3 s.
In general, as shown in all cases, big facets develop within
1 s, by consuming the small ones. This is consistent with the experimental observations [2]. Unfortunately, the step merging is
not through the step growth as observed in the experiment

結果 (中文) 3:

各向异性动力学函数，即，式（6），对于不同的D
值显示在图4（a），这表明峰值在451；
峰值给B 11¼5.1 S / M（N¼10）。较大的D值为
分布较窄。的界面形态结构演变
奥希斯（F¼0）基于D¼4，16，和64，分别在图4所示，
（b），（c）和（d）N 10、E 4¼¼0.25。小扰动
（40小波）介绍的开始。每个接口的间隔
0.22 s，总时间为3.3 s。
一般，在所有的案例中，在1大方面的发展
，消耗小的。这与实验结果是一致的[ 2 ]。不幸的是，步骤合并
不通过逐步增长的实验中观察到