Numerical schemes for a three component Cahn-Hilliard model

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Decoupled, Energy Stable Schemes for Phase-Field Models of Two-Phase Incompressible Flows (2015, methodology): “Recently, an interesting approach was proposed in [4, 26] to treat the difficulty (i), where an explicit stabilizing term is added to the convective velocity in the phase equation.”
The Cahn-Hilliard Equation with Logarithmic Potentials (2011, unknown): “, [8], [9], [10], [11], [12], [13], [14], [30], [31], [32], [33], [34], [50], [60], [77], [78], [79], [86], [87], [88], [89], [94], [111], [122], [124],”
Numerical approximations for the molecular beam epitaxial growth model based on the invariant energy quadratization method (2017, background): “ the above two approaches cannot be easily applied. First of all, even though the convex-concave decomposition can be applied to F 0 , it is not clear how to deal with the sixth order polynomial term [7]. Second, it is uncertain whether the solution of the system satises certain maximum principle so”