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The normal second derivative is recovered from the equation

Statement

Assume Countable Choice. Let n≥1 and give Rn its Euclidean metric (Rn as the set of functions n→R, and d1, d2, d∞ are metrics on it). In this item relabel its zero-based coordinates by xi:=x(i−1) for 1≤i≤n; Di and ei refer to these coordinates. Define the open half-space H:={x∈Rn:xn>0} and its boundary hyperplane ∂H={x∈Rn:xn=0}. For r>0, write Br(x0):={x:∣x−x0∣<r} (Open ball, closed ball and sphere in a metric space), so the boundary half-ball is Q={x:∣x−x0∣<r, xn>0} with (x0)n=0. Let u∈H01(H)∩Hloc2(H) be such that the tangential second derivatives DkDiu (k<n) and the derivatives DnDiu for i<n exist in Lloc2(H); suppose u solves Lu=f weakly on H with aij∈W1,∞(H) uniformly elliptic with constant θ, bi,c∈L∞(H) and f∈Lloc2(H) (Local weak solutions of a divergence-form operator). Then the missing normal derivative DnDnu exists in Lloc2(H) and satisfies throughout H, in the almost-everywhere strong form, DnDnu=1ann(−∑(i,j)≠(n,n)aijDiDju−∑i,j(Diaij)Dju+biDiu+cu−f) almost everywhere, with the pointwise bound ∣DnDnu∣≤θ−1(Ma∑(i,j)≠(n,n)∣DiDju∣+C(n)(M1+Mb)∣Du∣+Mc∣u∣+∣f∣) and the corresponding L2 estimate on each boundary half-ball Q=Br(x0)∩H, x0∈∂H, on which f and all the nonnormal second derivatives on the right are in L2(Q). In particular those hypotheses imply Dn2u∈L2(Q), with ∥Dn2u∥L2(Q)≤C(∑(i,j)≠(n,n)∥DiDju∥L2(Q)+∥Du∥L2(Q)+∥u∥L2(Q)+∥f∥L2(Q)). Uniform ellipticity gives Re⁡ann≥θ and hence ∣ann∣≥θ, which makes division legitimate for real or complex coefficients.

Facts & Assumptions

Given: Countable Choice; the half-space; the coefficient package; the data and the solution with the stated partial second derivatives.

[F1]

Local weak solution: a(u,φ)=∫Hfφ‾ dx for every φ∈Cc∞(H). (Local weak solutions of a divergence-form operator)

[F2]

Coefficient package: ∣aij∣≤Ma, ∣Diaij∣≤M1, ∣bi∣≤Mb, ∣c∣≤Mc a.e. and Re⁡(aijξjξi‾)≥θ∣ξ∣2; in particular Re⁡ann≥θ>0 and ∣ann∣≥θ a.e. (Uniformly elliptic divergence-form operators and their sesquilinear forms)

[F3]

On an open set where u is a strong solution, integration by parts in [F1] against φ∈Cc∞ gives ∫H(−Di(aijDju)+biDiu+cu−f)φ‾ dx=0 for every test function, where Di(aijDju)=(Diaij)Dju+aijDiDju with the displayed second derivatives integrable; since the bracket lies in Lloc2 and is orthogonal to every Cc∞ function, it vanishes a.e. (The notation Hk and the reserved zero-boundary symbol, Smooth compactly supported functions of an open set are dense in L2)

Proof

technique · direct
1.1F1F2F3

Strong identity in the open half-space. On every compactly contained open subset of H, the hypothesis u∈Hloc2(H) and the multiplier rule of The cutoff difference-quotient commutator estimate for a∈W1,∞ give Di(aijDju)=(Diaij)Dju+aijDiDju in L2. The weak equation and density of smooth tests imply −Di(aijDju)+biDiu+cu=f almost everywhere there. A countable exhaustion proves this identity almost everywhere throughout H; no boundary H2 regularity has been assumed.

2.1step 1.1F2algebra

Algebraic recovery. Separating the (n,n) term gives annDn2u=−∑(i,j)≠(n,n)aijDiDju−∑i,j(Diaij)Dju+biDiu+cu−f. Testing ellipticity with ξ=en gives Re⁡ann≥θ, hence ∣1/ann∣≤θ−1 even for complex coefficients. Division therefore gives the displayed formula and pointwise bound almost everywhere on H.

3.1step 2.1F2algebra

Estimate up to the flat boundary. Let Q=Br(x0)∩H be a boundary half-ball satisfying the integrability conditions in the Statement. The right-hand side of step 2.1 belongs to L2(Q) because the nonnormal derivatives and f do, and u∈H1(H). Integrating the pointwise bound over Q and using the triangle inequality proves the displayed L2(Q) estimate. The already existing interior weak derivative Dn2u equals this L2(Q) function on every compact test support in Q, so the same function represents that weak derivative on the entire open half-ball. This recovers boundary integrability without first assuming u∈H2(Q).

4.1step 2.1step 3.1∎

Conclusion. The equation determines the normal derivative throughout H and bounds it on every boundary half-ball where the tangential and mixed second derivatives and forcing have been controlled. Together with the tangential difference-quotient estimate, this supplies the missing second derivative up to the flat boundary for real or complex coefficients.

Source notes

Hunter (printed pp. 115-116) recovers ∂n2u from the equation after the tangential second derivatives have been estimated, and Teschl's Lemma 10.18 (printed p. 242) proceeds in the same order. The formula is the algebraic solve for annDnDnu in the strong form of the equation; the ellipticity bound ∣ann∣≥θ obtained from ξ=en is what makes the division legitimate.

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Sources