We simulate a finite system of N confined electrons with inclusion of the D
arwin magnetic interaction in two and three dimensions. The lowest-energy s
tates are located using the steepest descent quenching adapted for velocity
dependent potentials. Below a critical density the ground state is a stati
c Wigner lattice. For supercritical density the ground state has a nonzero
kinetic energy. The critical density decreases with N for exponential confi
nement but not for harmonic confinement. The lowest-energy state also depen
ds on the confinement and dimension: an antiferromagnetic cluster forms for
harmonic confinement in two dimensions.