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Proposition 3.9: energy-space local control

PDF p. 15: Proposition 3.9; PDF p. 16: proof concludes

Statement

Assume the Axiom of Choice and hypothesis (H): n∈{2,3}, Θ⊂Rn is nonempty and compact with smooth boundary, its exterior Ω=Rn∖Θ is connected, and every generalized reflected or glancing ray leaves each compact set in finite forward time. Let T>0, m∈{3,5} and λ∈R∖{0}. Choose the control cutoff φ of Control region and nested real cutoffs.

Let H01(Ω) be the closure of Cc∞(Ω;C) in H1(Ω), and let XT=C([0,T];H01(Ω))∩Lt4Lx∞, with compatible jointly measurable representatives and norm ∥v∥XT=sup⁡t∈[0,T]∥v(t)∥H1+∥v∥Lt4Lx∞. The mixed norm is the L4 norm in time of the spatial essential supremum. At s=1, this space satisfies the homogeneous, retarded-forcing and nonlinear estimates in the abstract perturbation hypotheses. After an equivalent constant rescaling of its norm if needed, it satisfies their norm-one inclusion convention as well.

Consequently, there is δ>0 such that for every v0,vT∈H01(Ω) with ∥v0∥H1,∥vT∥H1≤δ, there exist h∈C([0,T];H01(Ω)) and v∈XT solving i∂tv+ΔDv+λ∣v∣m−1v=φh in the integral sense, with v(0)=v0 and v(T)=vT. The homogeneous Dirichlet condition is encoded by ΔD. Thus the internally controlled system is locally exactly controllable in H01(Ω).

Facts & Assumptions

[F1]

The stated geometry and ray convention are those of Exterior and truncated obstacle domains. The cutoff and controlled equation are specified by Control region and nested real cutoffs and Linear and nonlinear internally controlled exterior systems. The stated Sobolev closure and scalar mixed-norm conventions are those of Complex integer-order Sobolev notation and Continuous and mixed time-space function spaces. The Axiom of Choice The Dirichlet operator is the realization in Dirichlet Laplacian and positive shift.

[F2]

Energy control space with a time-integrable supremum norm supplies completeness of XT with the displayed norm. Low-order identifications of the Dirichlet scale identifies HD1(Ω) and H01(Ω) as sets with equivalent norms.

[F3]

Under the stated geometry and Choice assumption, Free and retarded bounds in the energy control space gives the homogeneous evolution and retarded Bochner-forcing estimates in XT with H01 norms. Cubic and quintic energy-space nonlinear time estimates gives g(v)∈L1(0,T;H01) and the required growth and difference estimates for g(z)=λ∣z∣m−1z; its time factor is T(5−m)/4, including the value 1 for m=5.

[F4]

Abstract nonlinear control-space hypotheses specifies the Banach path space, norm-one inclusion and three estimates used by Theorem 3.7: abstract small-data perturbation result. That theorem gives a continuous control and an integral solution joining sufficiently small endpoints in HD1 when those hypotheses hold. The integral-solution convention and its mild equivalence are those of Mild formulation of the controlled power NLS.

Proof

Given: The assumptions and notation of the Statement.

Goal: Verify the abstract hypotheses at s=1 and obtain the stated local exact control.

1.1F2F4given

Put H=HD1(Ω). By F2, there are positive constants a,b such that a∥w∥H1≤∥w∥H≤b∥w∥H1 for every w∈H01. Choose c≥max⁡{1,b} and equip the same vector space XT with ∥v∥X^=c∥v∥XT. This equivalent norm preserves completeness, and sup⁡t∥v(t)∥H≤∥v∥X^. Hence the path-space and norm-one inclusion requirements in F4 hold.

2.1F2F3F4step 1.1

The homogeneous and retarded estimates of F3 apply to exactly this exterior, time interval and space. Replacing the H01 norms by the equivalent H norms and the XT norm by ∥⋅∥X^ changes only their constants. The same equivalence carries strong measurability and Bochner integrability between the two descriptions of H, so the forcing estimate has the required meaning. These are conditions (i) and (ii) of F4.

3.1F2F3F4step 1.1step 2.1

By F3, g(v) is Bochner integrable in H01 and satisfies the growth and difference bounds for every u,v∈XT. Norm equivalence and the rescaling in step 1.1 give the corresponding bounds with the H and X^ norms. Since T>0 is fixed, T(5−m)/4 is a finite constant, including when m=5. Taking one sufficiently large constant for these and the two linear bounds verifies condition (iii) and the common-constant requirement of F4.

4.1F1F2F4step 1.1step 2.1step 3.1∎

Apply the theorem in F4 with s=1 and the rescaled space. It yields a positive endpoint radius in the H norm, a control continuous in H, and an integral solution in XT with the prescribed endpoints. Choose δ small enough that bδ is at most that radius. The norm equivalence makes the control continuous in H01 and places every endpoint pair in the theorem's range, proving the stated conclusion.

Source notes

The frozen article is cited for attribution of Proposition 3.9. The application above uses the separately supplied linear and nonlinear estimates and the abstract control theorem; it does not use the article's proposition as a premise.

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