nLab quasiconformal map

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Differential geometry

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geometry of physics: coordinate systems, smooth spaces, manifolds, smooth homotopy types, supergeometry

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cohesion

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tangent cohesion

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graded differential cohesion

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id ⊣ id ∨ ∨ fermionic ⇉ ⊣ ⇝ bosonic ⊥ ⊥ bosonic ⇝ ⊣ Rh rheonomic ∨ ∨ reduced ℜ ⊣ ℑ infinitesimal ⊥ ⊥ infinitesimal ℑ ⊣ & étale ∨ ∨ cohesive ʃ ⊣ ♭ discrete ⊥ ⊥ discrete ♭ ⊣ ♯ continuous ∨ ∨ ∅ ⊣ * \array{ && id &\dashv& id \\ && \vee && \vee \\ &\stackrel{fermionic}{}& \rightrightarrows &\dashv& \rightsquigarrow & \stackrel{bosonic}{} \\ && \bot && \bot \\ &\stackrel{bosonic}{} & \rightsquigarrow &\dashv& \mathrm{R}\!\!\mathrm{h} & \stackrel{rheonomic}{} \\ && \vee && \vee \\ &\stackrel{reduced}{} & \Re &\dashv& \Im & \stackrel{infinitesimal}{} \\ && \bot && \bot \\ &\stackrel{infinitesimal}{}& \Im &\dashv& \& & \stackrel{\text{étale}}{} \\ && \vee && \vee \\ &\stackrel{cohesive}{}& \esh &\dashv& \flat & \stackrel{discrete}{} \\ && \bot && \bot \\ &\stackrel{discrete}{}& \flat &\dashv& \sharp & \stackrel{continuous}{} \\ && \vee && \vee \\ && \emptyset &\dashv& \ast }

Models

Lie theory, ∞-Lie theory

differential equations, variational calculus

Chern-Weil theory, ∞-Chern-Weil theory

Cartan geometry (super, higher)

Complex geometry

Contents

Definition

Consider

The ratio

(1)μ f≔∂¯f∂f \mu_f \coloneqq \frac { \bar\partial f } { \partial f }

of the function’s (anti-)holomorphic derivatives

∂f≔∂f∂z≔12(∂f∂x−i∂f∂y),∂¯f≔∂f∂z¯ \partial f \,\coloneqq\, \frac{\partial f}{\partial z} \;\coloneqq\; \tfrac{1}{2}\big( \tfrac{\partial f}{\partial x} -\mathrm{i} \tfrac{\partial f}{\partial y} \big) \,,\;\;\; \bar\partial f \,\coloneqq\, \frac{\partial f}{\partial \bar z}

is called the complex dilatation μ f\mu_f of ff, a measure for the function’s failure to be a conformal map or holomorphic map.

The actual dilatation of ff is defined to be the ratio

(2)D f≔1+d f1−d f D_f \;\coloneqq\; \frac { 1 + d_f } { 1 - d_f }

for

d f≔|μ f|=|∂¯f||∂f| d_f \;\coloneqq\; \left\vert\mu_f\right\vert = \frac { \left\vert \bar\partial f\right\vert } { \left\vert \partial f\right\vert }

the absolute value of the complex dilation (1).

The function ff is called quasi-conformal if its dilatation D f:ℂ⟶ℝD_f \colon \mathbb{C} \longrightarrow \mathbb{R} (2) is a bounded function.

References

  • Lars V. Ahlfors; pp. 4 of: Lectures on quasiconformal mappings, Van Nostrand, Princeton (1966), University Lecture Series 38 AMS (2006) [ams:ULECT/38, pdf]

  • Davoud Cheraghi; sections 7.1-2 in: Geometric Complex Analysis (2016) [pdf, Cheraghi-ComplexAnalysis.pdf?]

  • Nikolai V. Ivanov: The geometric meaning of the complex dilatation [arXiv:1701.06259]

See also:

Created on February 4, 2026 at 08:57:17. See the history of this page for a list of all contributions to it.