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TheoremStatement: Literature-sourcedProof: AI-adaptedPipeline-generatedprecheck passjudge pass (gpt-6.1-sol)audited 2026-10-08
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Every 1-quasiconformal homeomorphism is conformal

Statement

Assume the Axiom of Choice. Let Ω,Ω′⊆C be complex domains (A complex domain is a nonempty connected open subset of C) and f:Ω→Ω′ a homeomorphism. The following are equivalent.

(a) f is 1-quasiconformal, in either the geometric or the analytic sense (Orientation-preserving homeomorphisms and the geometric definition of quasiconformality, The ACL and Sobolev analytic definition of quasiconformality, The geometric and analytic definitions of quasiconformality agree).

(b) f∈Wloc1,2(Ω) and its weak Wirtinger derivative satisfies ∂zˉf=0 almost everywhere; under this Sobolev hypothesis this is equivalent to μf=0 almost everywhere together with ∂zˉf=0 almost everywhere on {∂zf=0} (The ACL and Sobolev analytic definition of quasiconformality, The Beltrami coefficient and the maximal dilatation).

(c) f is holomorphic; equivalently, it is a biholomorphism of Ω onto Ω′ (Biholomorphic maps between complex domains).

Thus the conformal maps in this library's orientation-preserving sense are exactly the 1-quasiconformal homeomorphisms; in particular, they preserve angles.

Facts & Assumptions

Given: Choice, complex domains Ω,Ω′, and a homeomorphism f:Ω→Ω′.

[F1]

The geometric and analytic definitions have the same least dilatation. In the analytic class, Kf=1 iff μf=0 almost everywhere; the defining inequality then gives fzˉ=0 almost everywhere. Conversely, if f is analytic quasiconformal and fzˉ=0 almost everywhere, then its Beltrami coefficient is zero (including the set where fz=0), so Kf=1 (The ACL and Sobolev analytic definition of quasiconformality, The Beltrami coefficient and the maximal dilatation, The geometric and analytic definitions of quasiconformality agree).

[F2]

Distributional derivatives commute, and Δ=4∂z∂zˉ on distributions (Linearity, locality, and commutation of weak derivatives, Distributional harmonicity and Poisson's equation on an open subset of Rn).

[F3]

A locally integrable distribution with zero Laplacian has a smooth harmonic representative; if the original function is continuous, it equals that representative everywhere (Weyl's lemma for the Laplacian, Locally integrable weakly harmonic functions are smooth).

[F4]

For a smooth function, the Cauchy–Riemann equation ∂zˉf=0 is equivalent to holomorphy. An injective holomorphic map on a complex domain has nowhere-vanishing derivative and a holomorphic inverse onto its open image (Complex differentiability is equivalent to real total differentiability together with a complex-linear derivative, with ∂zˉf=0, or with the Cauchy–Riemann equations, An injective holomorphic map has no critical point and is biholomorphic onto its image).

[F5]

At a differentiability point, a real-linear derivative given by multiplication by a nonzero complex number has determinant ∣f′(z)∣2>0 and hence preserves the local orientation (The Wirtinger derivatives ∂zf and ∂zˉf, and antiholomorphic functions, A real linear isomorphism preserves or reverses orientation according to the sign of its determinant, Smooth orientation sign is the local integral homology multiplier).

[F6]

A one-to-one holomorphic map preserves extremal length of every path family by conformal invariance, and thus satisfies the geometric modulus inequalities with constant 1 (Conformal invariance, monotonicity, and the series and parallel laws for extremal length, Orientation-preserving homeomorphisms and the geometric definition of quasiconformality).

Proof

technique · reduce the unit-dilatation condition to the weak Cauchy–Riemann equation, apply Weyl's lemma, and use conformal invariance for the converse
1.1F1given

By [F1], an analytically 1-quasiconformal map satisfies (b) and has μf=0 almost everywhere. If the hypothesis in (a) is geometric, the equivalence theorem first supplies the analytic condition with the same constant. Conversely, (b) is exactly the analytic 1-quasiconformal condition, so its least constant is 1. Under the Sobolev hypothesis, μf=0 forces fzˉ=0 off {fz=0}; the additional condition on that set gives fzˉ=0 almost everywhere, proving the coefficient reformulation in (b).

1.2F2given

Assume (b). The map f is continuous, hence locally integrable, and its weak Wirtinger derivative vanishes as a distribution. By [F2], Δf=4∂z(∂zˉf)=0 distributionally, componentwise.

2.1F3F4step 1.2given

By [F3], f agrees almost everywhere with a smooth harmonic function. The representative is actually f everywhere: the difference of two continuous functions that vanishes almost everywhere must vanish everywhere, since any point where it were nonzero would have a neighborhood of positive area where it remained nonzero. Thus f is smooth and harmonic. Its classical ∂zˉf is continuous and represents the zero distribution, so it vanishes pointwise; [F4] gives that f is holomorphic. Since f is injective, [F4] also shows its inverse is holomorphic onto its open image; surjectivity identifies that image with Ω′. Therefore f is a biholomorphism, proving (b)⇒(c).

3.1F1F4F5F6step 1.1step 1.2step 2.1given∎

Assume (c). Then f is injective and holomorphic, so [F4] gives f′(z)≠0 everywhere and a holomorphic inverse. By [F5], f preserves orientation. By [F6], it preserves the modulus of every quadrilateral family exactly, hence is geometrically 1-quasiconformal; the equivalence theorem in [F1] makes it analytically 1-quasiconformal as well. This proves (c)⇒(a); steps 1.1 and 1.2 prove (a)⇒(b), and step 2.1 proves (b)⇒(c).

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