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A function whose trace is at most a level has positive part in the zero-boundary space

Statement

Assume Countable Choice and the Axiom of Choice, inherited through the published trace and density suppliers named below. Let n≥2, let Ω⊂Rn be a bounded C1 domain (Bounded C^k domains and boundary charts), let u∈H1(Ω;R), and let T be the trace operator of The Lp trace operator on a bounded C1 domain. Then Tu≤0 a.e. on ∂Ω implies u+∈H01(Ω), and conversely u+∈H01(Ω) implies Tu≤0 a.e.; more generally, for every k∈R, (u−k)+∈H01(Ω) if and only if Tu≤k a.e. on ∂Ω. In particular the weak boundary order of Weak subsolutions and supersolutions of a divergence-form equation is the pointwise trace order, and the two conventions give the same boundary supremum sup⁡∂Ωu=ess sup⁡∂ΩTu (with value +∞ only if the trace is not essentially bounded above).

Facts & Assumptions

Given: Countable Choice and the Axiom of Choice; a bounded C1 domain Ω⊂Rn, n≥2; a real class u∈H1(Ω;R); the trace T; and a real level k.

[F1]

T:W1,2(Ω;R)→L2(∂Ω;R) is linear and bounded, and Tv=v∣∂Ω for every v∈C(Ω‾)∩H1(Ω) (The Lp trace operator on a bounded C1 domain, The trace agrees with classical restriction for continuous Sobolev functions).

[F2]

Assume the Axiom of Choice. Smooth functions on Ω‾ (restrictions of Cc∞(Rn) functions) are dense in H1(Ω), and Cc∞(Ω) is dense in H01(Ω) by definition (Ambient smooth restrictions are dense on bounded C^k domains, Zero-boundary Sobolev space as a norm closure).

[F3]

Assume the Axiom of Choice. {w∈H1(Ω):Tw=0}=H01(Ω) (The kernel of the trace is the closure of the test functions).

[F4]

Assume the Axiom of Choice. If w,wj∈H1(Ω;R) with wj→w in H1, then wj+→w+ in H1: pointwise ∣wj+−w+∣≤∣wj−w∣ and D(wj+−w+)=1{wj>0}Dwj−1{w>0}Dw=1{wj>0}D(wj−w)+(1{wj>0}−1{w>0})Dw, whose first term tends to 0 in L2. Every subsequence has a further subsequence with wj→w a.e.: choose the further terms with ∥wj−w∥22≤2−3j, so ∣{∣wj−w∣>2−j}∣≤2−j and countable subadditivity makes the limsup null. Along this further subsequence the indicator difference tends to zero where w≠0, while Dw=0 a.e. where w=0; dominated convergence with 4∣Dw∣2 makes the second term tend to zero in L2. If the full positive-part sequence did not converge, a subsequence with errors bounded below would contradict this argument. Therefore wj+→w+ in H1 (Positive-part truncation calculus and admissible cut-off weak tests, Positive, negative, and truncated Sobolev functions).

[F5]

Weak boundary order: u≤k on ∂Ω means (u−k)+∈H01(Ω), and sup⁡∂Ωu=inf⁡{k:u≤k on ∂Ω} with inf⁡∅=+∞ (Weak subsolutions and supersolutions of a divergence-form equation).

Proof

technique · direct; approximate by functions smooth up to the boundary, where the trace is the boundary restriction and commutes with truncation, then pass to the limit
1.1givenF1F2

Fix k∈R and put w:=u−k∈H1(Ω;R) and wk:=(u−k)+. By [F2] choose wj∈C∞(Ω‾) with wj→w in H1. For each j, wj+ is continuous on Ω‾ as the maximum of the continuous functions wj and 0, and it lies in H1(Ω) by the Lipschitz chain rule, so [F1] gives Twj+=wj+∣∂Ω=(wj∣∂Ω)+=(Twj)+ (the last equality using Twj=wj∣∂Ω from [F1]); moreover Twj→Tw in L2(∂Ω), so (Twj)+→(Tw)+ in L2(∂Ω) because t↦t+ is 1-Lipschitz on R.

2.1step 1.1F1F4

By [F4], wj+→w+ in H1(Ω), so the continuity of T in [F1] gives Twj+→Tw+ in L2(∂Ω). Since step 1.1 gives Twj+=(Twj)+→(Tw)+ in the same space, uniqueness of L2 limits yields T(w+)=(Tw)+ a.e. on ∂Ω.

3.1step 2.1F3algebra

Consequently, by [F3], w+∈H01(Ω)  ⟺  Tw+=0 in L2(∂Ω)  ⟺  (Tw)+=0 a.e.   ⟺  Tw≤0 a.e. on ∂Ω; since w=u−k and w+=(u−k)+, this is the asserted equivalence (u−k)+∈H01(Ω)  ⟺  Tu≤k a.e.

4.1step 3.1F3F5∎

The boundary supremum. By [F5] and step 3.1, the admissible levels are {k∈R:u≤k on ∂Ω}={k∈R:Tu≤k a.e.}=[ess sup⁡∂ΩTu,+∞) when the trace is essentially bounded above, and the empty set when it is not; the infimum is therefore ess sup⁡∂ΩTu in the first case and +∞ in the second, which proves the boundary-supremum identification. The argument uses only the declared Countable Choice and Axiom of Choice.

Depends on

Used by

Cited to discharge well-definedness by Weak subsolutions and supersolutions of a divergence-form equation.

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Sources