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C2 flattening preserves uniform ellipticity quantitatively

Statement

Assume Countable Choice. In the setting of Weak divergence-form equations are invariant under C2 boundary charts with W compactly contained in the domain of a flattening chart of a bounded C2 domain (Bounded C^k domains and boundary charts), suppose Λ≥1 bounds ∣DΦ∣,∣Dψ∣,∣det⁡DΦ∣ and ∣det⁡Dψ∣ together with their reciprocals on the relevant closure: Λ−1≤∣det⁡Dψ(y)∣≤Λ and ∣ζ∣≤Λ∣DΦ(ψ(y))ζ∣ for all ζ. Then the transformed coefficients a~ ij of Weak divergence-form equations are invariant under C2 boundary charts satisfy, for a.e. y in the flattened half-ball, Re⁡∑i,ja~ij(y)ξjξi‾ ≥ θ Λ−2inf⁡∣det⁡Dψ∣ ∣ξ∣2(ξ∈Cn), so the transformed operator is uniformly elliptic with an explicitly computable constant depending only on n,θ,Λ, while the transformed coefficients satisfy ∣a~ ij∣≤n2MaΛ3. The first-order and zero-order coefficients satisfy ∣b~ i∣≤nMbΛ2 and ∣c~∣≤McΛ, hence also the scaffold's non-sharp bounds C(n)(Ma+Mb)Λ3 for ∣b~ i∣ and C(n)(Ma+Mb+Mc)Λ3 for ∣c~∣, since Λ≥1. The constants are not asserted sharp. Ellipticity alone does not imply the coefficient regularity required for an H2 estimate. If additionally a∈W1,∞ on the original patch, then the transformed principal coefficients are W1,∞ on the compact half-patch, with bounds also depending on ∥Da∥∞ and the second chart/inverse derivatives.

Facts & Assumptions

Given: Countable Choice; the chart and its inverse with the two-sided bounds of the Statement; the coefficients aij,bi,c with ellipticity constant θ and bounds Ma,Mb,Mc; and the transformed coefficients of the boundary-chart lemma.

[F1]

Transformed coefficients: for a.e. y, a~ ij(y)=∣det⁡Dψ(y)∣∑p,qapq(ψ(y))∂pΦi(ψ(y))∂qΦj(ψ(y)), b~ i(y)=∣det⁡Dψ(y)∣∑pbp(ψ(y))∂pΦi(ψ(y)) and c~(y)=∣det⁡Dψ(y)∣c(ψ(y)). (Weak divergence-form equations are invariant under C2 boundary charts)

[F2]

Chart bounds: with Mip:=∂pΦi(ψ(y)) and N:=Dψ(y) one has MN=NM=I, ∣det⁡N∣≥Λ−1, ∣det⁡N∣≤Λ, and ∣MTξ∣≥Λ−1∣ξ∣ for every ξ. The latter follows because M and MT have the same singular values and the Statement bounds the smallest singular value of M below by Λ−1. (Bounded C^k domains and boundary charts)

[F3]

Uniform ellipticity of the original form: Re⁡(∑p,qapq(x)ζqζp‾)≥θ∣ζ∣2 for a.e. x and all ζ∈Cn. (Uniformly elliptic divergence-form operators and their sesquilinear forms)

Proof

1.1F2given

Setup. Fix y in the flattened half-ball and put Mip:=∂pΦi(ψ(y)), N:=Dψ(y) and ζ:=MTξ, so that ζp=∑iMipξi. By [F2] ∣ζ∣≥Λ−1∣ξ∣ and ∣det⁡N∣≥Λ−1>0.

1.2F1F2algebra

Coefficient bounds. From [F1], the coefficient bounds and [F2], ∣a~ ij∣≤∣det⁡N∣∑p,qMa∣Mip∣∣Mjq∣≤Λ⋅n2MaΛ2=n2MaΛ3, while ∣b~ i∣≤Λ⋅nMbΛ=nMbΛ2 and ∣c~∣≤ΛMc. Since Λ≥1 and Ma+Mb≥Mb, this implies the non-sharp bounds C(n)(Ma+Mb)Λ3 and C(n)(Ma+Mb+Mc)Λ3 for suitable C(n).

2.1F1step 1.1algebra

Quadratic form. Substituting the definition of a~ ij from [F1] and interchanging the finite sums gives ∑i,ja~ijξjξi‾=∣det⁡N∣∑p,qapq(∑jMjqξj)(∑iMipξi)‾=∣det⁡N∣∑p,qapqζqζp‾.

3.1F3step 1.1step 2.1algebra

Ellipticity. Taking real parts in step 2.1 and applying [F3] to ζ gives Re⁡∑i,ja~ijξjξi‾≥∣det⁡N∣ θ∣ζ∣2≥θ Λ−2inf⁡∣det⁡Dψ∣ ∣ξ∣2, where the last inequality uses ∣det⁡N∣≥inf⁡∣det⁡Dψ∣ and step 1.1.

4.1F1F2step 3.1step 1.2algebra∎

The transformed coefficients satisfy the stated ellipticity and size bounds. For the additional regularity clause, the first-order weak pullback formula follows by smooth approximation on compact interior subsets; change of variables and the compact ambient chart bounds bound the resulting derivative fields uniformly up to the flat boundary. Thus a∘ψ∈W1,∞ there. Apply the multiplier rule of The cutoff difference-quotient commutator estimate to the factors ∣det⁡Dψ∣, DΦ∘ψ and a∘ψ in [F1]. Their first derivatives use Da and the second chart/inverse derivatives, giving the asserted bounds. Flat-boundary H2 estimates require this additional regularity and admissible boundary data.

Source notes

Hunter (printed p. 114) performs the same substitution ζ=DΦTξ immediately after the coefficient formulas and notes that C2 boundary regularity is what makes the transformed coefficients C1; Teschl's Lemma 10.18 (printed p. 242) uses the same computation. The scaffold's displayed lower bound is reproduced in step 3.1; the sharper coefficient bounds in step 4.1 imply the scaffold's non-sharp versions.

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