As temperatures near the critical point, the interface between the liquid and gas phases becomes indistinct, rendering the configurations less precise. These mixed phases are labeled Coexist-Blur Morph in Figure , due to the presence of a minor volume of the vapor phase. Starting from lower temperatures and moving into this area, we notice a reduction in droplet phases at low densities (ρ * = 0.05 and 0.1). In contrast, at higher densities (ρ * = 0.6 and 0.67), the vapor phase diminishes, resulting in the transition from cylindrical to spherical bubble configurations. As expected, the configurations in these domains are less distinct.