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The elliptic adjoint gives the reduced parameter gradient

Statement

Assume Countable Choice and the elliptic state setting of Parameter-dependent coercive elliptic variational states and objectives and A uniformly coercive elliptic variational state is C1 in its parameter. Let J:V×Θ→R be C1. For a parameter θ, let pθ∈V solve the adjoint variational problem aθ(v,pθ)=DuJ(uθ,θ)[v](v∈V). Then the reduced objective j(θ)=J(uθ,θ) is C1 and Dθj(θ)[η]=DθJ(uθ,θ)[η]+Dθℓθ[η](pθ)−Dθaθ[η](uθ,pθ). No symmetry of aθ is required; the adjoint uses the transposed variational form displayed above.

Facts & Assumptions

Given: The uniformly coercive real variational state, its C1 dependence, the C1 objective, and Countable Choice.

[F1]

The state derivative wη is the unique solution of aθ(wη,v)=Dθℓθ[η](v)−Dθaθ[η](uθ,v) (A uniformly coercive elliptic variational state is C1 in its parameter).

[F2]

A bounded linear functional has a unique adjoint variational solution with aθ(v,p)=G(v) under Countable Choice (Well-posedness of the adjoint variational problem, The Axiom of Countable Choice (ACω)).

[F3]

The chain rule for Fr'echet differentiable maps between real Banach spaces gives D(J∘Γ)=DJ(Γ)DΓ (Chain sum product and composition rules for Banach derivatives).

[A1]

J and its first derivatives are continuous on the state/parameter neighborhood.

Proof

1.1F2A1given

The adjoint datum DuJ(uθ,θ) is a bounded linear functional on V. By [F2], the adjoint pθ exists uniquely, with the equation in the Statement.

1.2F1F2F3given

Let Γ(θ)=(uθ,θ). The state differentiability in [F1] gives DΓ(θ)[η]=(wη,η). Apply the Banach-space chain rule [F3] to j=J∘Γ to obtain Dθj[η]=DθJ(uθ,θ)[η]+DuJ(uθ,θ)[wη]. Since J and the state map are C1, this derivative is continuous, so j is C1. Use the adjoint equation with v=wη to replace the second term by aθ(wη,pθ).

2.1F1step 1.2

Use the state-sensitivity equation [F1] with test function v=pθ. It gives aθ(wη,pθ)=Dθℓθ[η](pθ)−Dθaθ[η](uθ,pθ).

3.1step 1.2step 2.1algebra∎

Substitute step 2.1 into step 1.2 to obtain the formula. The argument uses only the displayed adjoint equation, so it remains valid for a nonsymmetric coercive form.

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