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Interior H2 estimate for constant-coefficient elliptic equations

Statement

Assume Countable Choice. Let n≥1, K∈{R,C}, let aij∈K be a constant matrix satisfying Re⁡(∑aijξjξi‾)≥θ∣ξ∣2 with θ>0 and ∣aij∣≤Ma, let bi,c∈K be constants with ∣bi∣≤Mb, ∣c∣≤Mc, and let L be the associated constant-coefficient divergence-form operator with form a. Let f∈L2(BR(x0)) and let u∈H1(BR(x0)) solve Lu=f weakly on BR(x0). Then u∈H2(Br(x0)) for every 0<r<R, with ∥D2u∥L2(Br(x0))≤C((1+1(R−r)2)∥u∥L2(BR(x0))+∥f∥L2(BR(x0))), where C=C(n,θ,Ma,Mb,Mc). No symmetry of a and no boundary condition on u is required, and the estimate is the transparent constant-coefficient core of the variable-coefficient theorem.

Facts & Assumptions

Given: Countable Choice; the ball BR(x0) with 0<r<R; constant coefficients aij,bi,c with the bounds and ellipticity of the Statement; f∈L2(BR(x0)); and a local weak solution u∈H1(BR(x0)) of Lu=f.

[F1]

Local weak solution: a(u,φ)=∫BR(x0)fφ‾ dx for every φ∈Cc∞(BR(x0)). (Local weak solutions of a divergence-form operator)

[F2]

The constant-coefficient form and ellipticity: a(w,z)=∫(aijDjwDiz‾+biDiwz‾+cwz‾)dx with Re⁡(aijξjξi‾)≥θ∣ξ∣2, ∣bi∣≤Mb, ∣c∣≤Mc. (Uniformly elliptic divergence-form operators and their sesquilinear forms)

[F3]

Difference-quotient calculus: for locally integrable classes the two-domain integration-by-parts identity holds and reduces to ∫δhiw φ‾ dx=−∫w δ−hiφ‾ dx whenever the product has compact support of distance exceeding ∣h∣ from the boundary; the product rule δhi(wζ)=(τ−heiw)δhiζ+(δhiw)ζ holds; and difference quotients commute with weak derivatives, Dα(δhiw)=δhi(Dαw) on the shrunken domain. (Difference-quotient calculus: integration by parts, product rule, commutation)

[F4]

The localised test class: for u∈H1, η∈Cc∞ and 0<∣h∣<dist⁡(supp⁡η,∂Ω) the class v:=−δ−hk(η2δhku) lies in H01 and is an admissible test class in the weak equation. (The difference-quotient test function and its commutators)

[F5]

Scales: for every x0 and 0<r<R there is η∈Cc∞(B(r+R)/2(x0)) with 0≤η≤1, η=1 on Br(x0) and ∥Dη∥∞≤C(n)/(R−r); and the scaled Caccioppoli inequality holds on concentric balls Bρ(x0)⋐BR(x0). (The standard smooth step function, The chain rule for total derivatives: D(g∘f)(a)=Dg(f(a))∘Df(a), Compactly supported scaled Euclidean bumps, Scaled Caccioppoli inequality on concentric balls)

[F6]

Young and Cauchy--Schwarz: ab≤εa2+(4ε)−1b2 for ε>0 and real a,b≥0, and ∣∫gh‾ dx∣≤∥g∥L2∥h∥L2. (Young's inequality for conjugate real exponents, Holder's inequality for integrals, including the endpoint cases)

[F7]

Difference-quotient characterisation of W1,p for 1<p<∞: (1) if u∈W1,p(Ω) then ∥δhiu∥Lp(Ω′)≤∥Diu∥Lp(Ω) for 0<∣h∣<dist⁡(Ω′,∂Ω); (2) conversely, if ∥δhiu∥Lp(Ω′)≤C for all 0<∣h∣<dist⁡(Ω′,∂Ω)/2, then Diu∈Lp(Ω′) with ∥Diu∥Lp(Ω′)≤C. The weak-limit supplier proves the same converse from bounds for all 0<∣h∣<h0 for any finite positive h0 below the domain margin. (The difference-quotient characterisation of W1,p for 1<p<∞, Uniformly bounded difference quotients represent a weak derivative)

Proof

technique · direct
1.1F4F5

Setup. Fix x0 and 0<r<R, put ρ:=(r+R)/2 and h0:=(R−r)/4, and choose the real cutoff η(x)=σ((s∗2−∣x−x0∣2)/(s∗2−r2)) with s∗=(r+ρ)/2 and the fixed smooth step of [F5]. Its support lies in B‾s∗⋐Bρ, it equals one on Br, and the chain rule gives ∥Dη∥∞≤4∥σ′∥∞/(ρ−r)=C1/(R−r) with C1=8∥σ′∥∞, so that ∥D(η2)∥∞≤2C1/(R−r). For 0<∣h∣<h0 and k∈{1,…,n} the class v:=−δ−hk(η2δhku) is defined and admissible in the weak equation by [F4], and all difference quotients below are taken on Bρ(x0).

2.1F2F3step 1.1

Constant-coefficient translation. For w=η2δhku, its support and all small translates are compactly contained in BR. Discrete integration by parts and commutation of weak derivatives therefore give a(u,−δ−hkw)=a(δhku,w), since the coefficients are constant. This use is confined to the supported test w; an arbitrary H01(BR) test need not admit a translation staying inside the ball.

3.1F1F2F3F7step 2.1algebra

Expansion and datum. Put Eh=∥ηδhkDu∥2 and s=R−r. The product rule expands a(δhku,η2δhku) into the accretive principal term, the principal cutoff term, and drift/reaction terms. On the supported cutoff neighbourhood, with shifts remaining inside Bρ, the coordinate quotient bound gives ∥δhku∥2≤∥Dku∥L2(Bρ) after decreasing h0 to the cutoff-support margin if necessary. Thus ∥v∥2≤C(Eh+s−1∥Du∥L2(Bρ)). This only uses norms on valid shrunken domains, not an undefined quotient on all BR.

4.1F2F6step 3.1algebra

Absorption. The principal cutoff term is at most CMas−1Eh∥Du∥L2(Bρ). The drift and reaction terms are bounded by CMbEh∥Du∥L2(Bρ)+Mc∥Du∥L2(Bρ)2. The datum pairing is at most C∥f∥L2(BR)(Eh+s−1∥Du∥L2(Bρ)). Young's inequality and Re⁡Ph≥θEh2 therefore give Eh2≤C((1+s−2)∥Du∥L2(Bρ)2+∥f∥L2(BR)2), where C depends only on n,θ,Ma,Mb,Mc, uniformly in sufficiently small h.

5.1F1F2F5F6step 4.1algebra

Refined gradient estimate. To eliminate the intermediate gradient, choose a smooth cutoff β equal to one on Bρ, supported in BR with ∥Dβ∥∞≤C/s, and test the weak equation with β2u. The Caccioppoli computation behind [F5], taking real parts and absorbing the principal cutoff and drift products by Young, gives ∥Du∥L2(Bρ)2≤C((1+s−2)∥u∥L2(BR)2+∥f∥L2(BR)∥u∥L2(BR)). Set t=(1+s−2)−1 and use ∥f∥2∥u∥2≤t∥f∥22+(4t)−1∥u∥22. Then ∥Du∥L2(Bρ)2≤C((1+s−2)∥u∥22+(1+s−2)−1∥f∥22). Substituting this bound into step 4.1 yields Eh2≤C((1+s−2)2∥u∥22+∥f∥22). This retains the forcing coefficient at every scale.

6.1step 5.1F7algebra∎

Conclusion. Since η=1 on Br, step 5.1 bounds every coordinate quotient δhkDju on Br uniformly for all sufficiently small h. The converse criterion [F7], applied with any finite threshold below both this support margin and (R−r)/2, gives each DkDju∈L2(Br) with the same bound. Summing the finitely many second-derivative bounds and taking square roots gives the displayed estimate ∥D2u∥L2(Br)≤C((1+(R−r)−2)∥u∥L2(BR)+∥f∥L2(BR)).

Source notes

Laugesen's Theorem 5.6 (printed pp. 108-110) proves the estimate for L=−Δ by difference quotients with the cutoff test function, and Hunter's Theorem 4.27 (printed pp. 110-114) carries out the same scheme for general divergence-form operators; the constant-coefficient case has no coefficient commutators, so the error terms in step 3.1 contain only the cutoff gradients Di(η2), which is why the step-size h disappears from the final constant. The scaled Caccioppoli inequality supplies the (R−r)−2∥u∥L2(BR) term exactly at the scale of the statement.

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