A free-energy functional for a crystal that contains both the symmetry conserved and symmetry broken parts of the direct pair correlation function is developed. To test how accurately this free-energy functional describes the symmetry breaking first-order phase transition of freezing, we use it to investigate the crystallization of fluids interacting via the inverse power potential; u(r)=[?](s/r)n. In agreement with simulation results we find that under the fluid-solid co-existence the f.c.c. structure is more stable for n=12, whereas for soft repulsions (n[?] 6) the b.c.c. structure is more stable.