We discuss static and dynamic fluctuations of domain walls separating
areas of constant but different slopes in steady-state configurations
of crystalline surfaces both by an analytic treatment of the appropria
te Langevin equation and by numerical simulations. In contrast to othe
r situations that describe the dynamics in Ising-like systems such as
models A and B, we find that the dynamic exponent z = 2 that governs t
he domain wall relaxation function is not equal to the inverse of the
exponent n approximate to 1/4 that describes the coarsening process th
at leads to the steady state.