A tunable solid-on-solid model of surface growth

We have performed a detailed Monte Carlo study of a diffusionless $(1+1)$-dimensional solid-on-solid model of particle deposition and evaporation that not only tunes the roughness of an equilibrium surface but also demonstrates the need for more than two exponents to characterize it. The tunable parameter, denoted by $\mu$, in this model is the dimensionless surface tension per unit length. For $\mu <0$, the surface becomes increasingly spikier and its average width grows linearly with time; for $\mu =0$, its width grows as $\sqrt{t}$. On the other hand, for positive $\mu$, the surface width shows the standard scaling behavior, $\la \sigma_m(t)\ra \sim M^{\alpha}f(t/M^{\alpha /\beta})$where$M$isthesubstratesizeand$f(x) \to const (x^{\beta})$for$x$large(small)\mathrm{.}Theroughnessexponent,$\alpha = 1/2$for$\mu \leq 2$,and$ = 3/5, 4/5 & \sim 1$for$\mu = 5, 6 & 7$respectively;thegrowthexponent,$\beta = 1/4$for$\mu \leq 2$and$= 1/2$for$\mu > \sim 3.5$ respectively. These exponents are different from those of the height-difference correlation function,${\alpha }^{\mathrm{\prime }}=1\mathrm{/}2,{\beta }^{\mathrm{\prime }}=1\mathrm{/}4$ and $z^{\mathrm{\prime }}=2$, for higher values of $\mu$ suggesting thereby that the surface could be self-constraining.