The (011) surface of the naphthalene crystal structure is described by
a simple restricted solid-on-solid model that Is applicable to a wide
range of organic crystals. Despite the absence of next-nearest-neighb
or bonds. the phase diagram of the model exhibits, besides flat and ro
ugh phases, a disordered flat phase. Monte Carlo simulations confirm t
his phase diagram. The presence of a disordered hat phase explains the
sudden disappearance of the (011) facet in experimental growth shapes
of naphthalene. The type of step-free energy associated with surface
tilt decreases rapidly, at preroughening transitions. This leads to a
rapid decrease in the nucleation barrier, which results in a sudden en
hanced growth rate and, under certain conditions, to the complete disa
ppearance of this facet in growth shapes.