nLab quasiconformal map

Redirected from "quasiconformal mappings".

Context

Differential geometry

synthetic differential geometry

Introductions

from point-set topology to differentiable manifolds

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

Differentials

V-manifolds

smooth space

Tangency

The magic algebraic facts

Theorems

Axiomatics

cohesion

infinitesimal cohesion

tangent cohesion

differential cohesion

graded differential cohesion

singular cohesion

id id fermionic bosonic bosonic Rh rheonomic reduced infinitesimal infinitesimal & 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¯ff \mu_f \coloneqq \frac { \bar\partial f } { \partial f }

of the function’s (anti-)holomorphic derivatives

ffz12(fxify),¯ffz¯ \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 f1+d f1d 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:D_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.