“…As the full temporally-evolving Cahn-Hilliard equation with sinusoidal forcing preserves the mean concentration ⟨ψ⟩, it follows that ⟨δC⟩ = 0 for all time. Therefore the boundary conditions on δC(x, t) are either (i) periodic, with δC(η+L, t) = δC(η, t), or (ii) bounded, with δC → 0 as η → ∞ (and the same for the η-derivatives of δC) or In this paper, we deal with Case (i) only, for the following reasons: this case is simple, and it can be used to shed light on the numerical simulations below in Section V. Also, the analysis developed in Case (i) may be combined with the theory developed in Reference [21], such that Case (ii) may be considered an extension of Case (i). As such, we focus in the rest of this section on periodic perturbations, with mean zero, specifically,…”