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Resolvent adjoint transport to order minus two

Statement

Assume the Axiom of Choice. Let n≥2, and let Θ⊂Rn be a nonempty compact obstacle with smooth boundary and connected exterior Ω=Rn∖Θ. Assume it is nontrapping in the complete-ray sense: for every complete unit-speed admissible generalized reflected or glancing ray x:R→Ω‾ and every compact K⊂Rn, there is t≥0 with x(t)∉K. Let ΔD be the Dirichlet Laplacian and let HDs be the spectral Hilbert scale of A=I−ΔD, with negative orders identified by the L2(Ω) pivot antidual pairing. Let η∈Cc∞(Rn) be real, and write Kz=η(−ΔD−z)−1η on L2(Ω) whenever the resolvent exists.

There are C>0 and ϵ0>0, depending on the obstacle and η, such that for every real λ, 0<ϵ≤ϵ0, and either sign, K(λ±iϵ)2 extends uniquely to a bounded operator HD−2→HD−1 of norm at most C. For every z with Re⁡z<0, the same extension satisfies ∥Kz∥HD−2→HD−1≤C(1+∣Re⁡z∣)−1/2. The constants are uniform in the indicated parameters.

Facts & Assumptions

[F1]

The exterior Dirichlet realization is self-adjoint, with −ΔD≥0 Exterior Dirichlet realization, H² domain and form domain.

[F2]

The scale is the completion of the common spectral core; its negative spaces are isometrically the pivot antiduals of the corresponding positive spaces Dirichlet spectral Sobolev scale and duality, Positive spectral Hilbert scale: duality and interpolation.

[F3]

For a nonnegative smooth compactly supported cutoff χ, the imported cutoff resolvent estimate applies from HD1 to HD2, uniformly on the two squared-parameter families and with the stated negative-real-part decay Nontrapping cutoff resolvent estimates.

[F4]

Multiplication by a smooth compactly supported function is bounded on each HDs for −2≤s≤2; on negative orders it is defined by the pivot pairing with the conjugate multiplier Endpoint multiplier bounds extended to negative spectral orders.

[F5]

The self-adjoint Borel calculus identifies the adjoint of a bounded spectral multiplier with the multiplier by its complex conjugate Unbounded Borel functional calculus: domains, products, spectral mapping. The assumed Axiom of Choice supplies the choice hypotheses of the cited scale and calculus results The Axiom of Choice.

[F6]

The explicit smooth-cutoff construction gives ρ∈Cc∞(Rn) with 0≤ρ≤1, ρ=1 for ∣x∣≤1, and ρ=0 for ∣x∣≥2; for every R>0, ρ(x/R) is again smooth and compactly supported Explicit compactly supported smooth cutoffs.

[F7]

For B=−ΔD on the complex Hilbert space L2(Ω), the resolvent set ρ(B) consists of those z∈C for which zI−B:D(B)→L2(Ω) is bijective with bounded everywhere defined inverse RB(z)=(zI−B)−1; the spectrum is σ(B)=C∖ρ(B) Resolvent and spectrum of an unbounded operator. Since B−zI=−(zI−B), the inverse used here is (B−zI)−1=−RB(z), with the same resolvent set and the same operator norm.

Proof

Given: The geometry, nontrapping assumption, scale, cutoff and parameter ranges in the Statement.

Goal: Construct the stated negative-order extensions and prove their bounds.

1.1F3F4F6given

Since η has compact support, the increasing open balls Bm(0), m≥1, cover supp⁡η, and a finite subcover gives R>0 with supp⁡η⊂BR(0); if the support is empty, take R=1. Take ρ from [F6] and set χ(x)=ρ(x/R). Then χ∈Cc∞(Rn), 0≤χ≤1, and χ=1 on BR(0), an open neighborhood of supp⁡η. Thus ηχ=η. The imported estimate applied to χ at order s=1, together with the multiplier bounds on HD1 and HD2, gives ∥Kw∥HD1→HD2≤C for w=(λ±iϵ)2 in its stated parameter range, and ∥Kw∥HD1→HD2≤C(1+∣Re⁡w∣)−1/2 for Re⁡w<0. Indeed, on L2, Kw=Mη(χ(−ΔD−w)−1χ)Mη; bounded extensions give the same identity on HD1. The constants absorb the two multiplier norms.

1.2F1F5F7given

The spectrum of −ΔD lies in [0,∞). Every parameter in the Statement and its complex conjugate is therefore in the resolvent set: the squared parameter is nonreal unless λ=0, when it is −ϵ2<0. The Borel calculus gives ((−ΔD−z)−1)∗=(−ΔD−z‾)−1 on L2. Since η is real, Mη∗=Mη, so Kz∗=Kz‾ on L2. Both parameter families are closed under conjugation and preserve the stated bound.

2.1F2step 1.1step 1.2∎

For f∈HD−2 define a conjugate-linear functional on HD1 by v↦⟨f,Kz‾v⟩−2,2. Step 1.1 bounds its norm by ∥f∥HD−2∥Kz‾∥HD1→HD2. Pivot antiduality therefore gives a unique Tf∈HD−1 with ⟨Tf,v⟩−1,1=⟨f,Kz‾v⟩−2,2 and the same operator bound. For f∈L2 this pairing equals ⟨Kzf,v⟩2 by step 1.2, so T extends the original Kz. The spectral core is dense in HD−2 and lies in L2, making this extension unique. Applying the bounds of step 1.1 to z‾ proves both asserted estimates.

Source notes

The negative-order statement is a local adjoint consequence of the cited positive-order imported estimate. The imported supplier retains its own source attribution and reading limits; no negative-order estimate is attributed directly to that source here.

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Used by · 2

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