“…Hence, γ(r, ṽ, h) = κ(r, ṽ, h) for all (r, ṽ, h) ∈ V 1 . We obtain that the Lagrange multiplier κ(r, v, h) 24), and the definition of A(r, v, h, γ) ∈ R m×m in (3.23). Thus, replacing the Lagrange remainder terms appearing due to Taylor expansions on the right hand side of (3.34) by their corresponding integral representations, it follows that λre (r, v, h) ∈ R m and Λre (r, v, h) ∈ R m×ℓ depend continuously on (r, v, h) ∈ D as well.…”