General self-flattening surfaces

Recently Jeong and Kim [Phys. Rev. E {\bf 66}, 051605 (2002)] investigated the scaling properties of equilibrium self-flattening surfaces subject to a restricted curvature constraint. In one dimension (1D), they found numerically that the stationary roughness exponent $\alpha \approx 0.561$ and the window exponent $\delta \approx 0.423$. We present an analytic argument for general self-flattening surfaces in $D$ dimensions, leading to $\alpha=D\alpha_0 /(D+\alpha_0)$and$\delta=D/(D+\alpha_0)$where$\alpha_0$ is the roughness exponent for equilibrium surfaces without the self-flattening mechanism. In case of surfaces subject to a restricted curvature constraint, it is known exactly that ${\alpha }_0=3\mathrm{/}2$ in 1D, which leads to $\alpha =3\mathrm{/}5$ and $\delta =2\mathrm{/}5$. Small discrepancies between our analytic values and their numerical values may be attributed to finite size effects.