We study rigorously ground-state orderings of particles in one-dimensional
classical lattice gases with nonconvex interactions. Such systems serve as
models of adsorption on crystal surfaces. In the considered models, the ene
rgy of adsorbed particles is a sum of two components, each one representing
the energy of a one-dimensional lattice gas with two-body interactions in
one of the two orthogonal lattice directions. This feature reduces two-dime
nsional problems to one-dimensional ones. The interaction energy in each di
rection is assumed here to be repulsive and strictly convex only from dista
nce 2 on, while its value at distance 1 can be positive or negative, but cl
ose to zero. We show that if the decay rate of the interactions is fast eno
ugh, then particles form 2-particle lattice-connected aggregates (dimers) w
hich are distributed in the same most homogeneous way as particles whose in
teraction is strictly convex everywhere. Moreover, despite the lack of conv
exity, the density of particles vs. the chemical potential appears to be a
fractal curve known as the complete devil's staircase.