Figure 8
The numerical solutions of the OZ equations have been determined on a grid with 214 = 16 364 points and a width of Δr = σ/500, where σ is the hard core diameter. The parameters of the potentials are chosen so that they reproduce the cluster peak as discussed by Liu et al. (2005), caused by a long-range attractive interaction potential contribution. The solutions of the numerical OZ solver (dashed lines) overlay with the analytical solutions (solid lines). Therefore, the numerical OZ solver provides equivalent results to the analytical solutions. |