Figure 4
Free energies of the single-scale periodic structures in the infinite-c LP model: as ∊ is increased, the uniform liquid is the equilibrium phase until it reaches −8/135, at which point a first-order transition to the hexagonal structure occurs. This persists until ∊ reaches (63/2 + 14)/15 where the lamellar structure becomes the equilibrium phase. The gray region corresponds to the forbidden zone below the lower bound, calculated in Section 6.6. |