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A local Jacobian and energy bound for quasiconformal homeomorphisms

Statement

Assume the Axiom of Choice. Let Ω,Ω′⊆C be complex domains and let f:Ω→Ω′ be an orientation-preserving K-geometrically quasiconformal homeomorphism, where K≥1. Put k=(K−1)/(K+1). Write ∂zf,∂zˉf for its weak Wirtinger derivatives, Jf=∣∂zf∣2−∣∂zˉf∣2 for its Jacobian, and ∣Df∣HS for the Hilbert--Schmidt norm of its real weak derivative matrix. Then for every relatively compact Borel set E⊂Ω, ∫EJf dA≤λ2(f(E)),∫E∣Df∣HS2 dA≤2(1+k2)1−k2 λ2(f(E)).

Facts & Assumptions

Given: AC, the geometric K-QC homeomorphism and the relatively compact Borel set E.

[F1]

Geometric and analytic K-quasiconformality agree, so the weak Wirtinger derivatives exist and obey ∣fzˉ∣≤k∣fz∣ (The geometric and analytic definitions of quasiconformality agree, The ACL and Sobolev analytic definition of quasiconformality).

[F2]

The earlier full distortion wrapper proves ∣f(E)∣=∫EJf without assuming the present lemma or MRMT (An analytically quasiconformal homeomorphism distorts quadrilateral moduli by at most K, area clause). Its lower inequality suffices here.

[F3]

Expanding the Wirtinger identities gives ∣Df∣HS2=2(∣fz∣2+∣fzˉ∣2) and Jf=∣fz∣2−∣fzˉ∣2 (The Wirtinger derivatives ∂zf and ∂zˉf, and antiholomorphic functions).

Proof

technique · use the earlier proved planar area formula and the Beltrami energy algebra
1.1F1F2given

Apply [F1] to regard f as an analytic K-QC map. The exact Borel-set area formula in [F2] gives ∫EJf=∣f(E)∣, hence the claimed lower inequality. No unrecovered Gehring–Lehto source is used; the complete differentiability and signed-degree arguments are in the earlier12 suppliers.

2.1F1F3step 1.1algebra∎

The Beltrami bound gives Jf≥(1−k2)∣fz∣2, and [F3] gives ∣Df∣HS2≤2(1+k2)∣fz∣2≤2(1+k2)(1−k2)−1Jf. Integrate and use step 1.1 to obtain the stated constant.

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