“…First if m < +∞, since ρ 1,m +ρ 2,m solves (5.1), then it is unique and according to Proposition 5.2, p m := F m (ρ 1,m + ρ 2,m ) is in L 2 ((0, T ), H 1 (Ω)). Moreover, we have already shown in Theorem 2.3 that the pressure p ∞ associated to the constraint ρ 1,∞ + ρ 2,∞ 1 is in L 2 ((0, T ), H 1 (Ω)) and, according to [21], (ρ 1,∞ + ρ 2,∞ , p ∞ ) is unique. Then, for m ∈ [1, +∞], ρ i 1,m solves…”