Riemann mapping theorem

<h2 id="history">History</h2>
The theorem was stated (under the assumption that the <a href="/facts/Boundary_(topology)/WgdH18kp">boundary</a> of 
 
 
 
 U
 
 
 {\displaystyle U}
 
 is piecewise smooth) by <a href="/facts/Bernhard_Riemann/oV2fL0k8">Bernhard Riemann</a> in 1851 in his PhD thesis. <a href="/facts/Lars_Ahlfors/aukXlC2t">Lars Ahlfors</a> wrote once, concerning the original formulation of the theorem, that it was “ultimately formulated in terms which would defy any attempt of proof, even with modern methods”.<a class="footnote-ref" id="fnref:2" href="#fn:2">2</a> Riemann's flawed proof depended on the <a href="/facts/Dirichlet_principle/2PUtzTL8">Dirichlet principle</a> (which was named by Riemann himself), which was considered sound at the time. However, <a href="/facts/Karl_Weierstrass/4U8vdQzL">Karl Weierstrass</a> found that this principle was not universally valid. Later, <a href="/facts/David_Hilbert/1vhlHn4b">David Hilbert</a> was able to prove that, to a large extent, the Dirichlet principle is valid under the hypothesis that Riemann was working with. However, in order to be valid, the Dirichlet principle needs certain hypotheses concerning the boundary of 
 
 
 
 U
 
 
 {\displaystyle U}
 
 (namely, that it is a Jordan curve) which are not valid for simply connected <a href="/facts/Domain_(mathematical_analysis)/xT44oI3E">domains</a> in general.
The first rigorous proof of the theorem was given by <a href="/facts/William_Fogg_Osgood/1mTufCMj">William Fogg Osgood</a> in 1900. He proved the existence of <a href="/facts/Green%27s_functions/rKxKKPcp">Green's function</a> on arbitrary simply connected domains other than 
 
 
 
 
 C
 
 
 
 {\displaystyle \mathbb {C} }
 
 itself; this established the Riemann mapping theorem.<a class="footnote-ref" id="fnref:3" href="#fn:3">3</a>
<a href="/facts/Constantin_Carath%C3%A9odory/ERbINCUr">Constantin Carathéodory</a> gave another proof of the theorem in 1912, which was the first to rely purely on the methods of function theory rather than <a href="/facts/Potential_theory/3sXGIcDA">potential theory</a>.<a class="footnote-ref" id="fnref:4" href="#fn:4">4</a> His proof used Montel's concept of normal families, which became the standard method of proof in textbooks.<a class="footnote-ref" id="fnref:5" href="#fn:5">5</a> Carathéodory continued in 1913 by resolving the additional question of whether the Riemann mapping between the domains can be extended to a homeomorphism of the boundaries (see <a href="/facts/Carath%C3%A9odory%27s_theorem_(conformal_mapping)/P2Rf169y">Carathéodory's theorem</a>).<a class="footnote-ref" id="fnref:6" href="#fn:6">6</a>
Carathéodory's proof used <a href="/facts/Riemann_surface/qoj8ogv8">Riemann surfaces</a> and it was simplified by <a href="/facts/Paul_Koebe/USjBbV2Y">Paul Koebe</a> two years later in a way that did not require them. Another proof, due to <a href="/facts/Lip%C3%B3t_Fej%C3%A9r/ywd5gwsw">Lipót Fejér</a> and to <a href="/facts/Frigyes_Riesz/EN47QveQ">Frigyes Riesz</a>, was published in 1922 and it was rather shorter than the previous ones. In this proof, like in Riemann's proof, the desired mapping was obtained as the solution of an extremal problem. The Fejér–Riesz proof was further simplified by <a href="/facts/Alexander_Ostrowski/r45sj25p">Alexander Ostrowski</a> and by Carathéodory.<a class="footnote-ref" id="fnref:7" href="#fn:7">7</a>

<h2 id="importance">Importance</h2>
The following points detail the uniqueness and power of the Riemann mapping theorem:

<ul><li>Even relatively simple Riemann mappings (for example a map from the interior of a circle to the interior of a square) have no explicit formula using only <a href="/facts/Elementary_function/wVFyDwu8">elementary functions</a>.</li>
<li>Simply connected open sets in the plane can be highly complicated, for instance, the <a href="/facts/Boundary_(topology)/WgdH18kp">boundary</a> can be a nowhere-<a href="/facts/Differentiable_function/jQqTgLk1">differentiable</a> <a href="/facts/Fractal_curve/jjanzwda">fractal curve</a> of infinite length, even if the set itself is bounded. One such example is the <a href="/facts/Koch_curve/JTckxQVK">Koch curve</a>.<a class="footnote-ref" id="fnref:8" href="#fn:8">8</a> The fact that such a set can be mapped in an angle-preserving manner to the nice and regular unit disc seems counter-intuitive.</li>
<li>The analog of the Riemann mapping theorem for more complicated domains is not true. The next simplest case is of doubly connected domains (domains with a single hole). Any doubly connected domain except for the punctured disk and the punctured plane is conformally equivalent to some annulus 
 
 
 
 {
 z
 :
 r
 <
 
 |
 
 z
 
 |
 
 <
 1
 }
 
 
 {\displaystyle \{z:r<|z|<1\}}
 
 with 
 
 
 
 0
 <
 r
 <
 1
 
 
 {\displaystyle 0<r<1}
 
, however there are no conformal maps between <a href="/facts/Annulus_(mathematics)/rhxKuoem">annuli</a> except inversion and multiplication by constants so the annulus 
 
 
 
 {
 z
 :
 1
 <
 
 |
 
 z
 
 |
 
 <
 2
 }
 
 
 {\displaystyle \{z:1<|z|<2\}}
 
 is not conformally equivalent to the annulus 
 
 
 
 {
 z
 :
 1
 <
 
 |
 
 z
 
 |
 
 <
 4
 }
 
 
 {\displaystyle \{z:1<|z|<4\}}
 
 (as can be <a href="/facts/Extremal_length/MTNaUwlu">proven using extremal length</a>).</li>
<li>The analogue of the Riemann mapping theorem in three or more real dimensions is not true. The family of conformal maps in three dimensions is very poor, and essentially contains only <a href="/facts/M%C3%B6bius_transformation/YEkTTLfK">Möbius transformations</a> (see <a href="/facts/Liouville%27s_theorem_(conformal_mappings)/mXldCrcj"> Liouville's theorem</a>).</li>
<li>Even if arbitrary <a href="/facts/Homeomorphism/jMfWg3Mn">homeomorphisms</a> in higher dimensions are permitted, <a href="/facts/Contractible/REXYj8uS">contractible</a> <a href="/facts/Manifold/rXPERJtu">manifolds</a> can be found that are not homeomorphic to the <a href="/facts/Ball_(mathematics)/f9vpMVMp"> ball</a> (e.g., the <a href="/facts/Whitehead_continuum/JkRq8dzE">Whitehead continuum</a>).</li>
<li>The analogue of the Riemann mapping theorem in <a href="/facts/Function_of_several_complex_variables/axwNpV4a">several complex variables</a> is also not true. In 
 
 
 
 
 
 C
 
 
 n
 
 
 
 
 {\displaystyle \mathbb {C} ^{n}}
 
 (
 
 
 
 n
 ≥
 2
 
 
 {\displaystyle n\geq 2}
 
), the ball and <a href="/facts/Polydisk/p3Ivtu0W">polydisk</a> are both simply connected, but there is no biholomorphic map between them.<a class="footnote-ref" id="fnref:9" href="#fn:9">9</a></li></ul>
<h2 id="proof-via-normal-families">Proof via normal families</h2>
Main article: <a href="/facts/Normal_families/KlVUaMoj">Normal families</a>
<h3>Simple connectivity</h3>
Theorem. For an open domain 
 
 
 
 G
 ⊂
 
 C
 
 
 
 {\displaystyle G\subset \mathbb {C} }
 
 the following conditions are equivalent:<a class="footnote-ref" id="fnref:10" href="#fn:10">10</a>

<ol><li>
 
 
 
 G
 
 
 {\displaystyle G}
 
 is simply connected;</li>
<li>the integral of every holomorphic function 
 
 
 
 f
 
 
 {\displaystyle f}
 
 around a closed piecewise smooth curve in 
 
 
 
 G
 
 
 {\displaystyle G}
 
 vanishes;</li>
<li>every holomorphic function in 
 
 
 
 G
 
 
 {\displaystyle G}
 
 is the derivative of a holomorphic function;</li>
<li>every nowhere-vanishing holomorphic function 
 
 
 
 f
 
 
 {\displaystyle f}
 
 on 
 
 
 
 G
 
 
 {\displaystyle G}
 
 has a holomorphic logarithm;</li>
<li>every nowhere-vanishing holomorphic function 
 
 
 
 g
 
 
 {\displaystyle g}
 
 on 
 
 
 
 G
 
 
 {\displaystyle G}
 
 has a holomorphic square root;</li>
<li>for any 
 
 
 
 w
 ∉
 G
 
 
 {\displaystyle w\notin G}
 
, the <a href="/facts/Winding_number/kaquyUL2">winding number</a> of 
 
 
 
 w
 
 
 {\displaystyle w}
 
 for any piecewise smooth closed curve in 
 
 
 
 G
 
 
 {\displaystyle G}
 
 is 
 
 
 
 0
 
 
 {\displaystyle 0}
 
;</li>
<li>the complement of 
 
 
 
 G
 
 
 {\displaystyle G}
 
 in the extended complex plane 
 
 
 
 
 C
 
 ∪
 {
 ∞
 }
 
 
 {\displaystyle \mathbb {C} \cup \{\infty \}}
 
 is connected.</li></ol>
(1) ⇒ (2) because any continuous closed curve, with base point 
 
 
 
 a
 ∈
 G
 
 
 {\displaystyle a\in G}
 
, can be continuously deformed to the constant curve 
 
 
 
 a
 
 
 {\displaystyle a}
 
. So the line integral of 
 
 
 
 f
 
 
 d
 
 z
 
 
 {\displaystyle f\,\mathrm {d} z}
 
 over the curve is 
 
 
 
 0
 
 
 {\displaystyle 0}
 
.
(2) ⇒ (3) because the integral over any piecewise smooth path 
 
 
 
 γ
 
 
 {\displaystyle \gamma }
 
 from 
 
 
 
 a
 
 
 {\displaystyle a}
 
 to 
 
 
 
 z
 
 
 {\displaystyle z}
 
 can be used to define a primitive.
(3) ⇒ (4) by integrating 
 
 
 
 
 f
 
 −
 1
 
 
 
 
 d
 
 f
 
 /
 
 
 d
 
 z
 
 
 {\displaystyle f^{-1}\,\mathrm {d} f/\mathrm {d} z}
 
 along 
 
 
 
 γ
 
 
 {\displaystyle \gamma }
 
 from 
 
 
 
 a
 
 
 {\displaystyle a}
 
 to 
 
 
 
 x
 
 
 {\displaystyle x}
 
 to give a branch of the logarithm.
(4) ⇒ (5) by taking the square root as 
 
 
 
 g
 (
 z
 )
 =
 exp
 ⁡
 (
 f
 (
 x
 )
 
 /
 
 2
 )
 
 
 {\displaystyle g(z)=\exp(f(x)/2)}
 
 where 
 
 
 
 f
 
 
 {\displaystyle f}
 
 is a holomorphic choice of logarithm.
(5) ⇒ (6) because if 
 
 
 
 γ
 
 
 {\displaystyle \gamma }
 
 is a piecewise closed curve and 
 
 
 
 
 f
 
 n
 
 
 
 
 {\displaystyle f_{n}}
 
 are successive square roots of 
 
 
 
 z
 −
 w
 
 
 {\displaystyle z-w}
 
 for 
 
 
 
 w
 
 
 {\displaystyle w}
 
 outside 
 
 
 
 G
 
 
 {\displaystyle G}
 
, then the winding number of 
 
 
 
 
 f
 
 n
 
 
 ∘
 γ
 
 
 {\displaystyle f_{n}\circ \gamma }
 
 about 
 
 
 
 w
 
 
 {\displaystyle w}
 
 is 
 
 
 
 
 2
 
 n
 
 
 
 
 {\displaystyle 2^{n}}
 
 times the winding number of 
 
 
 
 γ
 
 
 {\displaystyle \gamma }
 
 about 
 
 
 
 0
 
 
 {\displaystyle 0}
 
. Hence the winding number of 
 
 
 
 γ
 
 
 {\displaystyle \gamma }
 
 about 
 
 
 
 w
 
 
 {\displaystyle w}
 
 must be divisible by 
 
 
 
 
 2
 
 n
 
 
 
 
 {\displaystyle 2^{n}}
 
 for all 
 
 
 
 n
 
 
 {\displaystyle n}
 
, so it must equal 
 
 
 
 0
 
 
 {\displaystyle 0}
 
.
(6) ⇒ (7) for otherwise the extended plane 
 
 
 
 
 C
 
 ∪
 {
 ∞
 }
 ∖
 G
 
 
 {\displaystyle \mathbb {C} \cup \{\infty \}\setminus G}
 
 can be written as the disjoint union of two open and closed sets 
 
 
 
 A
 
 
 {\displaystyle A}
 
 and 
 
 
 
 B
 
 
 {\displaystyle B}
 
 with 
 
 
 
 ∞
 ∈
 B
 
 
 {\displaystyle \infty \in B}
 
 and 
 
 
 
 A
 
 
 {\displaystyle A}
 
 bounded. Let 
 
 
 
 δ
 >
 0
 
 
 {\displaystyle \delta >0}
 
 be the shortest Euclidean distance between 
 
 
 
 A
 
 
 {\displaystyle A}
 
 and 
 
 
 
 B
 
 
 {\displaystyle B}
 
 and build a square grid on 
 
 
 
 
 C
 
 
 
 {\displaystyle \mathbb {C} }
 
 with length 
 
 
 
 δ
 
 /
 
 4
 
 
 {\displaystyle \delta /4}
 
 with a point 
 
 
 
 a
 
 
 {\displaystyle a}
 
 of 
 
 
 
 A
 
 
 {\displaystyle A}
 
 at the centre of a square. Let 
 
 
 
 C
 
 
 {\displaystyle C}
 
 be the compact set of the union of all squares with distance 
 
 
 
 ≤
 δ
 
 /
 
 4
 
 
 {\displaystyle \leq \delta /4}
 
 from 
 
 
 
 A
 
 
 {\displaystyle A}
 
. Then 
 
 
 
 C
 ∩
 B
 =
 ∅
 
 
 {\displaystyle C\cap B=\varnothing }
 
 and 
 
 
 
 ∂
 C
 
 
 {\displaystyle \partial C}
 
 does not meet 
 
 
 
 A
 
 
 {\displaystyle A}
 
 or 
 
 
 
 B
 
 
 {\displaystyle B}
 
: it consists of finitely many horizontal and vertical segments in 
 
 
 
 G
 
 
 {\displaystyle G}
 
 forming a finite number of closed rectangular paths 
 
 
 
 
 γ
 
 j
 
 
 ∈
 G
 
 
 {\displaystyle \gamma _{j}\in G}
 
. Taking 
 
 
 
 
 C
 
 i
 
 
 
 
 {\displaystyle C_{i}}
 
 to be all the squares covering 
 
 
 
 A
 
 
 {\displaystyle A}
 
, then 
 
 
 
 
 
 1
 
 2
 π
 
 
 
 
 ∫
 
 ∂
 C
 
 
 
 d
 
 
 a
 r
 g
 
 (
 z
 −
 a
 )
 
 
 {\displaystyle {\frac {1}{2\pi }}\int _{\partial C}\mathrm {d} \mathrm {arg} (z-a)}
 
 equals the sum of the winding numbers of 
 
 
 
 
 C
 
 i
 
 
 
 
 {\displaystyle C_{i}}
 
 
over 
 
 
 
 a
 
 
 {\displaystyle a}
 
, thus giving 
 
 
 
 1
 
 
 {\displaystyle 1}
 
. On the other hand the sum of the winding numbers of 
 
 
 
 
 γ
 
 j
 
 
 
 
 {\displaystyle \gamma _{j}}
 
 about 
 
 
 
 a
 
 
 {\displaystyle a}
 
 equals 
 
 
 
 1
 
 
 {\displaystyle 1}
 
. Hence the winding number of at least one of the 
 
 
 
 
 γ
 
 j
 
 
 
 
 {\displaystyle \gamma _{j}}
 
 about 
 
 
 
 a
 
 
 {\displaystyle a}
 
 is non-zero.
(7) ⇒ (1) This is a purely topological argument. Let 
 
 
 
 γ
 
 
 {\displaystyle \gamma }
 
 be a piecewise smooth closed curve based at 
 
 
 
 
 z
 
 0
 
 
 ∈
 G
 
 
 {\displaystyle z_{0}\in G}
 
. By approximation γ is in the same <a href="/facts/Homotopy/1nWrPxdj">homotopy</a> class as a rectangular path on the square grid of length 
 
 
 
 δ
 >
 0
 
 
 {\displaystyle \delta >0}
 
 based at 
 
 
 
 
 z
 
 0
 
 
 
 
 {\displaystyle z_{0}}
 
; such a rectangular path is determined by a succession of 
 
 
 
 N
 
 
 {\displaystyle N}
 
 consecutive directed vertical and horizontal sides. By induction on 
 
 
 
 N
 
 
 {\displaystyle N}
 
, such a path can be deformed to a constant path at a corner of the grid. If the path intersects at a point 
 
 
 
 
 z
 
 1
 
 
 
 
 {\displaystyle z_{1}}
 
, then it breaks up into two rectangular paths of length 
 
 
 
 <
 N
 
 
 {\displaystyle <N}
 
, and thus can be deformed to the constant path at 
 
 
 
 
 z
 
 1
 
 
 
 
 {\displaystyle z_{1}}
 
 by the induction hypothesis and elementary properties of the <a href="/facts/Fundamental_group/VyYtLqSP">fundamental group</a>. The reasoning follows a "northeast argument":<a class="footnote-ref" id="fnref:11" href="#fn:11">11</a><a class="footnote-ref" id="fnref:12" href="#fn:12">12</a> in the non self-intersecting path there will be a corner 
 
 
 
 
 z
 
 0
 
 
 
 
 {\displaystyle z_{0}}
 
 with largest real part (easterly) and then amongst those one with largest imaginary part (northerly). Reversing direction if need be, the path go from 
 
 
 
 
 z
 
 0
 
 
 −
 δ
 
 
 {\displaystyle z_{0}-\delta }
 
 to 
 
 
 
 
 z
 
 0
 
 
 
 
 {\displaystyle z_{0}}
 
 and then to 
 
 
 
 
 w
 
 0
 
 
 =
 
 z
 
 0
 
 
 −
 i
 n
 δ
 
 
 {\displaystyle w_{0}=z_{0}-in\delta }
 
 for 
 
 
 
 n
 ≥
 1
 
 
 {\displaystyle n\geq 1}
 
 and then goes leftwards to 
 
 
 
 
 w
 
 0
 
 
 −
 δ
 
 
 {\displaystyle w_{0}-\delta }
 
. Let 
 
 
 
 R
 
 
 {\displaystyle R}
 
 be the open rectangle with these vertices. The winding number of the path is 
 
 
 
 0
 
 
 {\displaystyle 0}
 
 for points to the right of the vertical segment from 
 
 
 
 
 z
 
 0
 
 
 
 
 {\displaystyle z_{0}}
 
 to 
 
 
 
 
 w
 
 0
 
 
 
 
 {\displaystyle w_{0}}
 
 and 
 
 
 
 −
 1
 
 
 {\displaystyle -1}
 
 for points to the right; and hence inside 
 
 
 
 R
 
 
 {\displaystyle R}
 
. Since the winding number is 
 
 
 
 0
 
 
 {\displaystyle 0}
 
 off 
 
 
 
 G
 
 
 {\displaystyle G}
 
, 
 
 
 
 R
 
 
 {\displaystyle R}
 
 lies in 
 
 
 
 G
 
 
 {\displaystyle G}
 
. If 
 
 
 
 z
 
 
 {\displaystyle z}
 
 is a point of the path, it must lie in 
 
 
 
 G
 
 
 {\displaystyle G}
 
; if 
 
 
 
 z
 
 
 {\displaystyle z}
 
 is on 
 
 
 
 ∂
 R
 
 
 {\displaystyle \partial R}
 
 but not on the path, by continuity the winding number of the path about 
 
 
 
 z
 
 
 {\displaystyle z}
 
 is 
 
 
 
 −
 1
 
 
 {\displaystyle -1}
 
, so 
 
 
 
 z
 
 
 {\displaystyle z}
 
 must also lie in 
 
 
 
 G
 
 
 {\displaystyle G}
 
. Hence 
 
 
 
 R
 ∪
 ∂
 R
 ⊂
 G
 
 
 {\displaystyle R\cup \partial R\subset G}
 
. But in this case the path can be deformed by replacing the three sides of the rectangle by the fourth, resulting in two less sides (with self-intersections permitted).

<h3>Riemann mapping theorem</h3>
<ul><li>Weierstrass' convergence theorem. The uniform limit on compacta of a sequence of holomorphic functions is holomorphic; similarly for derivatives.</li></ul>
This is an immediate consequence of <a href="/facts/Morera%27s_theorem/vqw1Pvu8">Morera's theorem</a> for the first statement. <a href="/facts/Cauchy%27s_integral_formula/4B35nkvV">Cauchy's integral formula</a> gives a formula for the derivatives which can be used to check that the derivatives also converge uniformly on compacta.<a class="footnote-ref" id="fnref:13" href="#fn:13">13</a>
<ul><li><a href="/facts/Hurwitz%27s_theorem_(complex_analysis)/Fm8wIUW0">Hurwitz's theorem</a>. If a sequence of nowhere-vanishing holomorphic functions on an open domain has a uniform limit on compacta, then either the limit is identically zero or the limit is nowhere-vanishing. If a sequence of univalent holomorphic functions on an open domain has a uniform limit on compacta, then either the limit is constant or the limit is univalent.</li></ul>
If the limit function is non-zero, then its zeros have to be isolated. Zeros with multiplicities can be counted by the winding number 
 
 
 
 
 
 1
 
 2
 π
 i
 
 
 
 
 ∫
 
 C
 
 
 
 g
 
 −
 1
 
 
 (
 z
 )
 
 g
 ′
 
 (
 z
 )
 
 d
 
 z
 
 
 {\displaystyle {\frac {1}{2\pi i}}\int _{C}g^{-1}(z)g'(z)\mathrm {d} z}
 
 for a holomorphic function 
 
 
 
 g
 
 
 {\displaystyle g}
 
. Hence winding numbers are continuous under uniform limits, so that if each function in the sequence has no zeros nor can the limit. For the second statement suppose that 
 
 
 
 f
 (
 a
 )
 =
 f
 (
 b
 )
 
 
 {\displaystyle f(a)=f(b)}
 
 and set 
 
 
 
 
 g
 
 n
 
 
 (
 z
 )
 =
 
 f
 
 n
 
 
 (
 z
 )
 −
 
 f
 
 n
 
 
 (
 a
 )
 
 
 {\displaystyle g_{n}(z)=f_{n}(z)-f_{n}(a)}
 
. These are nowhere-vanishing on a disk but 
 
 
 
 g
 (
 z
 )
 =
 f
 (
 z
 )
 −
 f
 (
 a
 )
 
 
 {\displaystyle g(z)=f(z)-f(a)}
 
 vanishes at 
 
 
 
 b
 
 
 {\displaystyle b}
 
, so 
 
 
 
 g
 
 
 {\displaystyle g}
 
 must vanish identically.<a class="footnote-ref" id="fnref:14" href="#fn:14">14</a>
Definitions. A family 
 
 
 
 
 
 F
 
 
 
 
 {\displaystyle {\cal {F}}}
 
 of holomorphic functions on an open domain is said to be normal if any sequence of functions in 
 
 
 
 
 
 F
 
 
 
 
 {\displaystyle {\cal {F}}}
 
 has a subsequence that converges to a holomorphic function uniformly on compacta. 
A family 
 
 
 
 
 
 F
 
 
 
 
 {\displaystyle {\cal {F}}}
 
 is compact if whenever a sequence 
 
 
 
 
 f
 
 n
 
 
 
 
 {\displaystyle f_{n}}
 
 lies in 
 
 
 
 
 
 F
 
 
 
 
 {\displaystyle {\cal {F}}}
 
 and converges uniformly to 
 
 
 
 f
 
 
 {\displaystyle f}
 
 on compacta, then 
 
 
 
 f
 
 
 {\displaystyle f}
 
 also lies in 
 
 
 
 
 
 F
 
 
 
 
 {\displaystyle {\cal {F}}}
 
. A family 
 
 
 
 
 
 F
 
 
 
 
 {\displaystyle {\cal {F}}}
 
 is said to be locally bounded if their functions are uniformly bounded on each compact disk. Differentiating the <a href="/facts/Cauchy_integral_formula/4B35nkvV">Cauchy integral formula</a>, it follows that the derivatives of a locally bounded family are also locally bounded.<a class="footnote-ref" id="fnref:15" href="#fn:15">15</a><a class="footnote-ref" id="fnref:16" href="#fn:16">16</a>

<ul><li><a href="/facts/Montel%27s_theorem/JtG0GBXE">Montel's theorem</a>. Every locally bounded family of holomorphic functions in a domain 
 
 
 
 G
 
 
 {\displaystyle G}
 
 is normal.</li></ul>
Let 
 
 
 
 
 f
 
 n
 
 
 
 
 {\displaystyle f_{n}}
 
 be a totally bounded sequence and chose a countable dense subset 
 
 
 
 
 w
 
 m
 
 
 
 
 {\displaystyle w_{m}}
 
 of 
 
 
 
 G
 
 
 {\displaystyle G}
 
. By locally boundedness and a "diagonal argument", a subsequence can be chosen so that 
 
 
 
 
 g
 
 n
 
 
 
 
 {\displaystyle g_{n}}
 
 is convergent at each point 
 
 
 
 
 w
 
 m
 
 
 
 
 {\displaystyle w_{m}}
 
. It must be verified that this sequence of holomorphic functions converges on 
 
 
 
 G
 
 
 {\displaystyle G}
 
 uniformly on each compactum 
 
 
 
 K
 
 
 {\displaystyle K}
 
. Take 
 
 
 
 E
 
 
 {\displaystyle E}
 
 open with 
 
 
 
 K
 ⊂
 E
 
 
 {\displaystyle K\subset E}
 
 such that the closure of 
 
 
 
 E
 
 
 {\displaystyle E}
 
 is compact and contains 
 
 
 
 G
 
 
 {\displaystyle G}
 
. Since the sequence 
 
 
 
 {
 
 g
 
 n
 
 ′
 
 }
 
 
 {\displaystyle \{g_{n}'\}}
 
 is locally bounded, 
 
 
 
 
 |
 
 
 g
 
 n
 
 ′
 
 
 |
 
 ≤
 M
 
 
 {\displaystyle |g_{n}'|\leq M}
 
 on 
 
 
 
 E
 
 
 {\displaystyle E}
 
. By compactness, if 
 
 
 
 δ
 >
 0
 
 
 {\displaystyle \delta >0}
 
 is taken small enough, finitely many open disks 
 
 
 
 
 D
 
 k
 
 
 
 
 {\displaystyle D_{k}}
 
 of radius 
 
 
 
 δ
 >
 0
 
 
 {\displaystyle \delta >0}
 
 are required to cover 
 
 
 
 K
 
 
 {\displaystyle K}
 
 while remaining in 
 
 
 
 E
 
 
 {\displaystyle E}
 
. Since

g
          
            n
          
        
        (
        b
        )
        −
        
          g
          
            n
          
        
        (
        a
        )
        =
        
          ∫
          
            a
          
          
            b
          
        
        
          g
          
            n
          
          
            ′
          
        
        (
        z
        )
        
        d
        z
      
    
    {\displaystyle g_{n}(b)-g_{n}(a)=\int _{a}^{b}g_{n}^{\prime }(z)\,dz}
  
,
we have that 
  
    
      
        
          |
        
        
          g
          
            n
          
        
        (
        a
        )
        −
        
          g
          
            n
          
        
        (
        b
        )
        
          |
        
        ≤
        M
        
          |
        
        a
        −
        b
        
          |
        
        ≤
        2
        δ
        M
      
    
    {\displaystyle |g_{n}(a)-g_{n}(b)|\leq M|a-b|\leq 2\delta M}
  
. Now for each 
  
    
      
        k
      
    
    {\displaystyle k}
  
 choose some 
  
    
      
        
          w
          
            i
          
        
      
    
    {\displaystyle w_{i}}
  
 in 
  
    
      
        
          D
          
            k
          
        
      
    
    {\displaystyle D_{k}}
  
 where 
  
    
      
        
          g
          
            n
          
        
        (
        
          w
          
            i
          
        
        )
      
    
    {\displaystyle g_{n}(w_{i})}
  
 converges, take 
  
    
      
        n
      
    
    {\displaystyle n}
  
 and 
  
    
      
        m
      
    
    {\displaystyle m}
  
 so large to be within 
  
    
      
        δ
      
    
    {\displaystyle \delta }
  
 of its limit. Then for 
  
    
      
        z
        ∈
        
          D
          
            k
          
        
      
    
    {\displaystyle z\in D_{k}}
  
,

|
        
        
          g
          
            n
          
        
        (
        z
        )
        −
        
          g
          
            m
          
        
        (
        z
        )
        
          |
        
        ≤
        
          |
        
        
          g
          
            n
          
        
        (
        z
        )
        −
        
          g
          
            n
          
        
        (
        
          w
          
            i
          
        
        )
        
          |
        
        +
        
          |
        
        
          g
          
            n
          
        
        (
        
          w
          
            i
          
        
        )
        −
        
          g
          
            m
          
        
        (
        
          w
          
            i
          
        
        )
        
          |
        
        +
        
          |
        
        
          g
          
            m
          
        
        (
        
          w
          
            1
          
        
        )
        −
        
          g
          
            m
          
        
        (
        z
        )
        
          |
        
        ≤
        4
        M
        δ
        +
        2
        δ
        .
      
    
    {\displaystyle |g_{n}(z)-g_{m}(z)|\leq |g_{n}(z)-g_{n}(w_{i})|+|g_{n}(w_{i})-g_{m}(w_{i})|+|g_{m}(w_{1})-g_{m}(z)|\leq 4M\delta +2\delta .}

Hence the sequence 
 
 
 
 {
 
 g
 
 n
 
 
 }
 
 
 {\displaystyle \{g_{n}\}}
 
 forms a Cauchy sequence in the uniform norm on 
 
 
 
 K
 
 
 {\displaystyle K}
 
 as required.<a class="footnote-ref" id="fnref:17" href="#fn:17">17</a><a class="footnote-ref" id="fnref:18" href="#fn:18">18</a>
<ul><li>Riemann mapping theorem. If 
 
 
 
 G
 ≠
 
 C
 
 
 
 {\displaystyle G\neq \mathbb {C} }
 
 is a simply connected domain and 
 
 
 
 a
 ∈
 G
 
 
 {\displaystyle a\in G}
 
, there is a unique conformal mapping 
 
 
 
 f
 
 
 {\displaystyle f}
 
 of 
 
 
 
 G
 
 
 {\displaystyle G}
 
 onto the unit disk 
 
 
 
 D
 
 
 {\displaystyle D}
 
 normalized such that 
 
 
 
 f
 (
 a
 )
 =
 0
 
 
 {\displaystyle f(a)=0}
 
 and 
 
 
 
 
 f
 ′
 
 (
 a
 )
 >
 0
 
 
 {\displaystyle f'(a)>0}
 
.</li></ul>
Uniqueness follows because if 
 
 
 
 f
 
 
 {\displaystyle f}
 
 and 
 
 
 
 g
 
 
 {\displaystyle g}
 
 satisfied the same conditions, 
 
 
 
 h
 =
 f
 ∘
 
 g
 
 −
 1
 
 
 
 
 {\displaystyle h=f\circ g^{-1}}
 
 would be a univalent holomorphic map of the unit disk with 
 
 
 
 h
 (
 0
 )
 =
 0
 
 
 {\displaystyle h(0)=0}
 
 and 
 
 
 
 
 h
 ′
 
 (
 0
 )
 >
 0
 
 
 {\displaystyle h'(0)>0}
 
. But by the <a href="/facts/Schwarz_lemma/70DeQvPJ">Schwarz lemma</a>, the univalent holomorphic maps of the unit disk onto itself are given by the <a href="/facts/M%C3%B6bius_transformation/YEkTTLfK">Möbius transformations</a>

k
        (
        z
        )
        =
        
          e
          
            i
            θ
          
        
        (
        z
        −
        α
        )
        
          /
        
        (
        1
        −
        
          
            α
            ¯
          
        
        z
        )
      
    
    {\displaystyle k(z)=e^{i\theta }(z-\alpha )/(1-{\overline {\alpha }}z)}

with 
 
 
 
 
 |
 
 α
 
 |
 
 <
 1
 
 
 {\displaystyle |\alpha |<1}
 
. So 
 
 
 
 h
 
 
 {\displaystyle h}
 
 must be the identity map and 
 
 
 
 f
 =
 g
 
 
 {\displaystyle f=g}
 
.
To prove existence, take 
 
 
 
 
 
 F
 
 
 
 
 {\displaystyle {\cal {F}}}
 
 to be the family of holomorphic univalent mappings 
 
 
 
 f
 
 
 {\displaystyle f}
 
 of 
 
 
 
 G
 
 
 {\displaystyle G}
 
 into the open unit disk 
 
 
 
 D
 
 
 {\displaystyle D}
 
 with 
 
 
 
 f
 (
 a
 )
 =
 0
 
 
 {\displaystyle f(a)=0}
 
 and 
 
 
 
 
 f
 ′
 
 (
 a
 )
 >
 0
 
 
 {\displaystyle f'(a)>0}
 
. It is a normal family by Montel's theorem. By the characterization of simple-connectivity, for 
 
 
 
 b
 ∈
 
 C
 
 ∖
 G
 
 
 {\displaystyle b\in \mathbb {C} \setminus G}
 
 there is a holomorphic branch of the square root 
 
 
 
 h
 (
 z
 )
 =
 
 
 z
 −
 b
 
 
 
 
 {\displaystyle h(z)={\sqrt {z-b}}}
 
 in 
 
 
 
 G
 
 
 {\displaystyle G}
 
. It is univalent and 
 
 
 
 h
 (
 
 z
 
 1
 
 
 )
 ≠
 −
 h
 (
 
 z
 
 2
 
 
 )
 
 
 {\displaystyle h(z_{1})\neq -h(z_{2})}
 
 for 
 
 
 
 
 z
 
 1
 
 
 ,
 
 z
 
 2
 
 
 ∈
 G
 
 
 {\displaystyle z_{1},z_{2}\in G}
 
. Since 
 
 
 
 h
 (
 G
 )
 
 
 {\displaystyle h(G)}
 
 must contain a closed disk 
 
 
 
 Δ
 
 
 {\displaystyle \Delta }
 
 with centre 
 
 
 
 h
 (
 a
 )
 
 
 {\displaystyle h(a)}
 
 and radius 
 
 
 
 r
 >
 0
 
 
 {\displaystyle r>0}
 
, no points of 
 
 
 
 −
 Δ
 
 
 {\displaystyle -\Delta }
 
 can lie in 
 
 
 
 h
 (
 G
 )
 
 
 {\displaystyle h(G)}
 
. Let 
 
 
 
 F
 
 
 {\displaystyle F}
 
 be the unique Möbius transformation taking 
 
 
 
 
 C
 
 ∖
 −
 Δ
 
 
 {\displaystyle \mathbb {C} \setminus -\Delta }
 
 onto 
 
 
 
 D
 
 
 {\displaystyle D}
 
 with the normalization 
 
 
 
 F
 (
 h
 (
 a
 )
 )
 =
 0
 
 
 {\displaystyle F(h(a))=0}
 
 and 
 
 
 
 (
 F
 ∘
 h
 
 )
 ′
 
 (
 a
 )
 =
 
 F
 ′
 
 (
 h
 (
 a
 )
 )
 ⋅
 
 h
 ′
 
 (
 a
 )
 >
 0
 
 
 {\displaystyle (F\circ h)'(a)=F'(h(a))\cdot h'(a)>0}
 
. By construction 
 
 
 
 F
 ∘
 h
 
 
 {\displaystyle F\circ h}
 
 is in 
 
 
 
 
 
 F
 
 
 
 
 {\displaystyle {\cal {F}}}
 
, so that 
 
 
 
 
 
 F
 
 
 
 
 {\displaystyle {\cal {F}}}
 
 is non-empty. The method of <a href="/facts/Paul_Koebe/USjBbV2Y">Koebe</a> is to use an extremal function to produce a conformal mapping solving the problem: in this situation it is often called the Ahlfors function of G, after <a href="/facts/Lars_Ahlfors/aukXlC2t">Ahlfors</a>.<a class="footnote-ref" id="fnref:19" href="#fn:19">19</a> Let 
 
 
 
 0
 <
 M
 ≤
 ∞
 
 
 {\displaystyle 0<M\leq \infty }
 
 be the supremum of 
 
 
 
 
 f
 ′
 
 (
 a
 )
 
 
 {\displaystyle f'(a)}
 
 for 
 
 
 
 f
 ∈
 
 
 F
 
 
 
 
 {\displaystyle f\in {\cal {F}}}
 
. Pick 
 
 
 
 
 f
 
 n
 
 
 ∈
 
 
 F
 
 
 
 
 {\displaystyle f_{n}\in {\cal {F}}}
 
 with 
 
 
 
 
 f
 
 n
 
 ′
 
 (
 a
 )
 
 
 {\displaystyle f_{n}'(a)}
 
 tending to 
 
 
 
 M
 
 
 {\displaystyle M}
 
. By Montel's theorem, passing to a subsequence if necessary, 
 
 
 
 
 f
 
 n
 
 
 
 
 {\displaystyle f_{n}}
 
 tends to a holomorphic function 
 
 
 
 f
 
 
 {\displaystyle f}
 
 uniformly on compacta. By Hurwitz's theorem, 
 
 
 
 f
 
 
 {\displaystyle f}
 
 is either univalent or constant. But 
 
 
 
 f
 
 
 {\displaystyle f}
 
 has 
 
 
 
 f
 (
 a
 )
 =
 0
 
 
 {\displaystyle f(a)=0}
 
 and 
 
 
 
 
 f
 ′
 
 (
 a
 )
 >
 0
 
 
 {\displaystyle f'(a)>0}
 
. So 
 
 
 
 M
 
 
 {\displaystyle M}
 
 is finite, equal to 
 
 
 
 
 f
 ′
 
 (
 a
 )
 >
 0
 
 
 {\displaystyle f'(a)>0}
 
 and 
 
 
 
 
 f
 ∈
 
 
 F
 
 
 
 
 
 {\displaystyle {f\in {\cal {F}}}}
 
. It remains to check that the conformal mapping 
 
 
 
 f
 
 
 {\displaystyle f}
 
 takes 
 
 
 
 G
 
 
 {\displaystyle G}
 
 onto 
 
 
 
 D
 
 
 {\displaystyle D}
 
. If not, take 
 
 
 
 c
 ≠
 0
 
 
 {\displaystyle c\neq 0}
 
 in 
 
 
 
 D
 ∖
 f
 (
 G
 )
 
 
 {\displaystyle D\setminus f(G)}
 
 and let 
 
 
 
 H
 
 
 {\displaystyle H}
 
 be a holomorphic square root of 
 
 
 
 (
 f
 (
 z
 )
 −
 c
 )
 
 /
 
 (
 1
 −
 
 
 c
 ¯
 
 
 f
 (
 z
 )
 )
 
 
 {\displaystyle (f(z)-c)/(1-{\overline {c}}f(z))}
 
 on 
 
 
 
 G
 
 
 {\displaystyle G}
 
. The function 
 
 
 
 H
 
 
 {\displaystyle H}
 
 is univalent and maps 
 
 
 
 G
 
 
 {\displaystyle G}
 
 into 
 
 
 
 D
 
 
 {\displaystyle D}
 
. Let

F
        (
        z
        )
        =
        
          
            
              
                e
                
                  i
                  θ
                
              
              (
              H
              (
              z
              )
              −
              H
              (
              a
              )
              )
            
            
              1
              −
              
                
                  
                    H
                    (
                    a
                    )
                  
                  ¯
                
              
              H
              (
              z
              )
            
          
        
        ,
      
    
    {\displaystyle F(z)={\frac {e^{i\theta }(H(z)-H(a))}{1-{\overline {H(a)}}H(z)}},}

where 
  
    
      
        
          H
          ′
        
        (
        a
        )
        
          /
        
        
          |
        
        
          H
          ′
        
        (
        a
        )
        
          |
        
        =
        
          e
          
            −
            i
            θ
          
        
      
    
    {\displaystyle H'(a)/|H'(a)|=e^{-i\theta }}
  
. Then 
  
    
      
        F
        ∈
        
          
            F
          
        
      
    
    {\displaystyle F\in {\cal {F}}}
  
 and a routine computation shows that

F
          ′
        
        (
        a
        )
        =
        
          H
          ′
        
        (
        a
        )
        
          /
        
        (
        1
        −
        
          |
        
        H
        (
        a
        )
        
          
            |
          
          
            2
          
        
        )
        =
        
          f
          ′
        
        (
        a
        )
        
          (
          
            
              
                
                  |
                
                c
                
                  |
                
              
            
            +
            
              
                
                  |
                
                c
                
                  
                    |
                  
                  
                    −
                    1
                  
                
              
            
          
          )
        
        
          /
        
        2
        >
        
          f
          ′
        
        (
        a
        )
        =
        M
        .
      
    
    {\displaystyle F'(a)=H'(a)/(1-|H(a)|^{2})=f'(a)\left({\sqrt {|c|}}+{\sqrt {|c|^{-1}}}\right)/2>f'(a)=M.}

This contradicts the maximality of 
 
 
 
 M
 
 
 {\displaystyle M}
 
, so that 
 
 
 
 f
 
 
 {\displaystyle f}
 
 must take all values in 
 
 
 
 D
 
 
 {\displaystyle D}
 
.<a class="footnote-ref" id="fnref:20" href="#fn:20">20</a><a class="footnote-ref" id="fnref:21" href="#fn:21">21</a><a class="footnote-ref" id="fnref:22" href="#fn:22">22</a>
Remark. As a consequence of the Riemann mapping theorem, every simply connected domain in the plane is homeomorphic to the unit disk. If points are omitted, this follows from the theorem. For the whole plane, the homeomorphism 
 
 
 
 ϕ
 (
 z
 )
 =
 z
 
 /
 
 (
 1
 +
 
 |
 
 z
 
 |
 
 )
 
 
 {\displaystyle \phi (z)=z/(1+|z|)}
 
 gives a homeomorphism of 
 
 
 
 
 C
 
 
 
 {\displaystyle \mathbb {C} }
 
 onto 
 
 
 
 D
 
 
 {\displaystyle D}
 
.

<h3>Parallel slit mappings</h3>
Koebe's uniformization theorem for normal families also generalizes to yield uniformizers 
 
 
 
 f
 
 
 {\displaystyle f}
 
 for multiply-connected domains to finite parallel slit domains, where the slits have angle 
 
 
 
 θ
 
 
 {\displaystyle \theta }
 
 to the x-axis. Thus if 
 
 
 
 G
 
 
 {\displaystyle G}
 
 is a domain in 
 
 
 
 
 C
 
 ∪
 {
 ∞
 }
 
 
 {\displaystyle \mathbb {C} \cup \{\infty \}}
 
 containing 
 
 
 
 ∞
 
 
 {\displaystyle \infty }
 
 and bounded by finitely many Jordan contours, there is a unique univalent function 
 
 
 
 f
 
 
 {\displaystyle f}
 
 on 
 
 
 
 G
 
 
 {\displaystyle G}
 
 with

f
        (
        z
        )
        =
        
          z
          
            −
            1
          
        
        +
        
          a
          
            1
          
        
        z
        +
        
          a
          
            2
          
        
        
          z
          
            2
          
        
        +
        ⋯
      
    
    {\displaystyle f(z)=z^{-1}+a_{1}z+a_{2}z^{2}+\cdots }

near 
 
 
 
 ∞
 
 
 {\displaystyle \infty }
 
, maximizing 
 
 
 
 
 R
 e
 
 (
 
 e
 
 −
 2
 i
 θ
 
 
 
 a
 
 1
 
 
 )
 
 
 {\displaystyle \mathrm {Re} (e^{-2i\theta }a_{1})}
 
 and having image 
 
 
 
 f
 (
 G
 )
 
 
 {\displaystyle f(G)}
 
 a parallel slit domain with angle 
 
 
 
 θ
 
 
 {\displaystyle \theta }
 
 to the x-axis.<a class="footnote-ref" id="fnref:23" href="#fn:23">23</a><a class="footnote-ref" id="fnref:24" href="#fn:24">24</a><a class="footnote-ref" id="fnref:25" href="#fn:25">25</a>
The first proof that parallel slit domains were canonical domains for in the multiply connected case was given by <a href="/facts/David_Hilbert/1vhlHn4b">David Hilbert</a> in 1909. Jenkins (1958), on his book on univalent functions and conformal mappings, gave a treatment based on the work of <a href="/facts/Herbert_Gr%C3%B6tzsch/aDQtE0hR">Herbert Grötzsch</a> and <a href="/facts/Ren%C3%A9_de_Possel/IWCjBzFx">René de Possel</a> from the early 1930s; it was the precursor of <a href="/facts/Quasiconformal_mapping/gICCqYEb">quasiconformal mappings</a> and <a href="/facts/Quadratic_differential/BP5o0MVR">quadratic differentials</a>, later developed as the technique of <a href="/facts/Extremal_length/MTNaUwlu">extremal metric</a> due to <a href="/facts/Oswald_Teichm%C3%BCller/s5YCszDf">Oswald Teichmüller</a>.<a class="footnote-ref" id="fnref:26" href="#fn:26">26</a> <a href="/facts/Menahem_Max_Schiffer/2Bt9THVw">Menahem Schiffer</a> gave a treatment based on very general <a href="/facts/Variational_principle/a5UkKEBj">variational principles</a>, summarised in addresses he gave to the <a href="/facts/International_Congress_of_Mathematicians/qQX4kVpe">International Congress of Mathematicians</a> in 1950 and 1958. In a theorem on "boundary variation" (to distinguish it from "interior variation"), he derived a differential equation and inequality, that relied on a measure-theoretic characterisation of straight-line segments due to Ughtred Shuttleworth Haslam-Jones from 1936. Haslam-Jones' proof was regarded as difficult and was only given a satisfactory proof in the mid-1970s by Schober and Campbell–Lamoureux.<a class="footnote-ref" id="fnref:27" href="#fn:27">27</a><a class="footnote-ref" id="fnref:28" href="#fn:28">28</a><a class="footnote-ref" id="fnref:29" href="#fn:29">29</a>
Schiff (1993) gave a proof of uniformization for parallel slit domains which was similar to the Riemann mapping theorem. To simplify notation, horizontal slits will be taken. Firstly, by <a href="/facts/Koebe_quarter_theorem/IAyU9SWC">Bieberbach's inequality</a>, any univalent function

g
        (
        z
        )
        =
        z
        +
        c
        
          z
          
            2
          
        
        +
        ⋯
      
    
    {\displaystyle g(z)=z+cz^{2}+\cdots }

with 
 
 
 
 z
 
 
 {\displaystyle z}
 
 in the open unit disk must satisfy 
 
 
 
 
 |
 
 c
 
 |
 
 ≤
 2
 
 
 {\displaystyle |c|\leq 2}
 
. As a consequence, if

f
        (
        z
        )
        =
        z
        +
        
          a
          
            0
          
        
        +
        
          a
          
            1
          
        
        
          z
          
            −
            1
          
        
        +
        ⋯
      
    
    {\displaystyle f(z)=z+a_{0}+a_{1}z^{-1}+\cdots }

is univalent in 
 
 
 
 
 |
 
 z
 
 |
 
 >
 R
 
 
 {\displaystyle |z|>R}
 
, then 
 
 
 
 
 |
 
 f
 (
 z
 )
 −
 
 a
 
 0
 
 
 
 |
 
 ≤
 2
 
 |
 
 z
 
 |
 
 
 
 {\displaystyle |f(z)-a_{0}|\leq 2|z|}
 
. To see this, take 
 
 
 
 S
 >
 R
 
 
 {\displaystyle S>R}
 
 and set

g
        (
        z
        )
        =
        S
        (
        f
        (
        S
        
          /
        
        z
        )
        −
        b
        
          )
          
            −
            1
          
        
      
    
    {\displaystyle g(z)=S(f(S/z)-b)^{-1}}

for 
 
 
 
 z
 
 
 {\displaystyle z}
 
 in the unit disk, choosing 
 
 
 
 b
 
 
 {\displaystyle b}
 
 so the denominator is nowhere-vanishing, and apply the <a href="/facts/Schwarz_lemma/70DeQvPJ">Schwarz lemma</a>. Next the function 
 
 
 
 
 f
 
 R
 
 
 (
 z
 )
 =
 z
 +
 
 R
 
 2
 
 
 
 /
 
 z
 
 
 {\displaystyle f_{R}(z)=z+R^{2}/z}
 
 is characterized by an "extremal condition" as the unique univalent function in 
 
 
 
 z
 >
 R
 
 
 {\displaystyle z>R}
 
 of the form 
 
 
 
 z
 +
 
 a
 
 1
 
 
 
 z
 
 −
 1
 
 
 +
 ⋯
 
 
 {\displaystyle z+a_{1}z^{-1}+\cdots }
 
 that maximises 
 
 
 
 
 R
 e
 
 (
 
 a
 
 1
 
 
 )
 
 
 {\displaystyle \mathrm {Re} (a_{1})}
 
: this is an immediate consequence of <a href="/facts/Koebe_quarter_theorem/IAyU9SWC">Grönwall's area theorem</a>, applied to the family of univalent functions 
 
 
 
 f
 (
 z
 R
 )
 
 /
 
 R
 
 
 {\displaystyle f(zR)/R}
 
 in 
 
 
 
 z
 >
 1
 
 
 {\displaystyle z>1}
 
.<a class="footnote-ref" id="fnref:30" href="#fn:30">30</a><a class="footnote-ref" id="fnref:31" href="#fn:31">31</a>
To prove now that the multiply connected domain 
 
 
 
 G
 ⊂
 
 C
 
 ∪
 {
 ∞
 }
 
 
 {\displaystyle G\subset \mathbb {C} \cup \{\infty \}}
 
 can be uniformized by a horizontal parallel slit conformal mapping

f
 (
 z
 )
 =
 z
 +
 
 a
 
 1
 
 
 
 z
 
 −
 1
 
 
 +
 ⋯
 
 
 {\displaystyle f(z)=z+a_{1}z^{-1}+\cdots }
 
,
take 
 
 
 
 R
 
 
 {\displaystyle R}
 
 large enough that 
 
 
 
 ∂
 G
 
 
 {\displaystyle \partial G}
 
 lies in the open disk 
 
 
 
 
 |
 
 z
 
 |
 
 <
 R
 
 
 {\displaystyle |z|<R}
 
. For 
 
 
 
 S
 >
 R
 
 
 {\displaystyle S>R}
 
, univalency and the estimate 
 
 
 
 
 |
 
 f
 (
 z
 )
 
 |
 
 ≤
 2
 
 |
 
 z
 
 |
 
 
 
 {\displaystyle |f(z)|\leq 2|z|}
 
 imply that, if 
 
 
 
 z
 
 
 {\displaystyle z}
 
 lies in 
 
 
 
 G
 
 
 {\displaystyle G}
 
 with 
 
 
 
 
 |
 
 z
 
 |
 
 ≤
 S
 
 
 {\displaystyle |z|\leq S}
 
, then 
 
 
 
 
 |
 
 f
 (
 z
 )
 
 |
 
 ≤
 2
 S
 
 
 {\displaystyle |f(z)|\leq 2S}
 
. Since the family of univalent 
 
 
 
 f
 
 
 {\displaystyle f}
 
 are locally bounded in 
 
 
 
 G
 ∖
 {
 ∞
 }
 
 
 {\displaystyle G\setminus \{\infty \}}
 
, by Montel's theorem they form a normal family. Furthermore if 
 
 
 
 
 f
 
 n
 
 
 
 
 {\displaystyle f_{n}}
 
 is in the family and tends to 
 
 
 
 f
 
 
 {\displaystyle f}
 
 uniformly on compacta, then 
 
 
 
 f
 
 
 {\displaystyle f}
 
 is also in the family and each coefficient of the Laurent expansion at 
 
 
 
 ∞
 
 
 {\displaystyle \infty }
 
 of the 
 
 
 
 
 f
 
 n
 
 
 
 
 {\displaystyle f_{n}}
 
 tends to the corresponding coefficient of 
 
 
 
 f
 
 
 {\displaystyle f}
 
. This applies in particular to the coefficient: so by compactness there is a univalent 
 
 
 
 f
 
 
 {\displaystyle f}
 
 which maximizes 
 
 
 
 
 R
 e
 
 (
 
 a
 
 1
 
 
 )
 
 
 {\displaystyle \mathrm {Re} (a_{1})}
 
. To check that

f
        (
        z
        )
        =
        z
        +
        
          a
          
            1
          
        
        +
        ⋯
      
    
    {\displaystyle f(z)=z+a_{1}+\cdots }

is the required parallel slit transformation, suppose reductio ad absurdum that 
 
 
 
 f
 (
 G
 )
 =
 
 G
 
 1
 
 
 
 
 {\displaystyle f(G)=G_{1}}
 
 has a compact and connected component 
 
 
 
 K
 
 
 {\displaystyle K}
 
 of its boundary which is not a horizontal slit. Then the complement 
 
 
 
 
 G
 
 2
 
 
 
 
 {\displaystyle G_{2}}
 
 of 
 
 
 
 K
 
 
 {\displaystyle K}
 
 in 
 
 
 
 
 C
 
 ∪
 {
 ∞
 }
 
 
 {\displaystyle \mathbb {C} \cup \{\infty \}}
 
 is simply connected with 
 
 
 
 
 G
 
 2
 
 
 ⊃
 
 G
 
 1
 
 
 
 
 {\displaystyle G_{2}\supset G_{1}}
 
. By the Riemann mapping theorem there is a conformal mapping

h
        (
        w
        )
        =
        w
        +
        
          b
          
            1
          
        
        
          w
          
            −
            1
          
        
        +
        ⋯
        ,
      
    
    {\displaystyle h(w)=w+b_{1}w^{-1}+\cdots ,}

such that 
 
 
 
 h
 (
 
 G
 
 2
 
 
 )
 
 
 {\displaystyle h(G_{2})}
 
 is 
 
 
 
 
 C
 
 
 
 {\displaystyle \mathbb {C} }
 
 with a horizontal slit removed. So we have that

h
        (
        f
        (
        z
        )
        )
        =
        z
        +
        (
        
          a
          
            1
          
        
        +
        
          b
          
            1
          
        
        )
        
          z
          
            −
            1
          
        
        +
        ⋯
        ,
      
    
    {\displaystyle h(f(z))=z+(a_{1}+b_{1})z^{-1}+\cdots ,}

and thus 
 
 
 
 
 R
 e
 
 (
 
 a
 
 1
 
 
 +
 
 b
 
 1
 
 
 )
 ≤
 
 R
 e
 
 (
 
 a
 
 1
 
 
 )
 
 
 {\displaystyle \mathrm {Re} (a_{1}+b_{1})\leq \mathrm {Re} (a_{1})}
 
 by the extremality of 
 
 
 
 f
 
 
 {\displaystyle f}
 
. Therefore, 
 
 
 
 
 R
 e
 
 (
 
 b
 
 1
 
 
 )
 ≤
 0
 
 
 {\displaystyle \mathrm {Re} (b_{1})\leq 0}
 
. On the other hand by the Riemann mapping theorem there is a conformal mapping

k
        (
        w
        )
        =
        w
        +
        
          c
          
            0
          
        
        +
        
          c
          
            1
          
        
        
          w
          
            −
            1
          
        
        +
        ⋯
        ,
      
    
    {\displaystyle k(w)=w+c_{0}+c_{1}w^{-1}+\cdots ,}

mapping from 
 
 
 
 
 |
 
 w
 
 |
 
 >
 S
 
 
 {\displaystyle |w|>S}
 
 onto 
 
 
 
 
 G
 
 2
 
 
 
 
 {\displaystyle G_{2}}
 
. Then

f
        (
        k
        (
        w
        )
        )
        −
        
          c
          
            0
          
        
        =
        w
        +
        (
        
          a
          
            1
          
        
        +
        
          c
          
            1
          
        
        )
        
          w
          
            −
            1
          
        
        +
        ⋯
        .
      
    
    {\displaystyle f(k(w))-c_{0}=w+(a_{1}+c_{1})w^{-1}+\cdots .}

By the strict maximality for the slit mapping in the previous paragraph, we can see that 
 
 
 
 
 R
 e
 
 (
 
 c
 
 1
 
 
 )
 <
 
 R
 e
 
 (
 
 b
 
 1
 
 
 +
 
 c
 
 1
 
 
 )
 
 
 {\displaystyle \mathrm {Re} (c_{1})<\mathrm {Re} (b_{1}+c_{1})}
 
, so that 
 
 
 
 
 R
 e
 
 (
 
 b
 
 1
 
 
 )
 >
 0
 
 
 {\displaystyle \mathrm {Re} (b_{1})>0}
 
. The two inequalities for 
 
 
 
 
 R
 e
 
 (
 
 b
 
 1
 
 
 )
 
 
 {\displaystyle \mathrm {Re} (b_{1})}
 
 are contradictory.<a class="footnote-ref" id="fnref:32" href="#fn:32">32</a><a class="footnote-ref" id="fnref:33" href="#fn:33">33</a><a class="footnote-ref" id="fnref:34" href="#fn:34">34</a>
The proof of the uniqueness of the conformal parallel slit transformation is given in Goluzin (1969) and Grunsky (1978). Applying the inverse of the <a href="/facts/Joukowsky_transform/gwtd93m9">Joukowsky transform</a> 
 
 
 
 h
 
 
 {\displaystyle h}
 
 to the horizontal slit domain, it can be assumed that 
 
 
 
 G
 
 
 {\displaystyle G}
 
 is a domain bounded by the unit circle 
 
 
 
 
 C
 
 0
 
 
 
 
 {\displaystyle C_{0}}
 
 and contains analytic arcs 
 
 
 
 
 C
 
 i
 
 
 
 
 {\displaystyle C_{i}}
 
 and isolated points (the images of other the inverse of the Joukowsky transform under the other parallel horizontal slits). Thus, taking a fixed 
 
 
 
 a
 ∈
 G
 
 
 {\displaystyle a\in G}
 
, there is a univalent mapping

F
          
            0
          
        
        (
        w
        )
        =
        h
        ∘
        f
        (
        w
        )
        =
        (
        w
        −
        a
        
          )
          
            −
            1
          
        
        +
        
          a
          
            1
          
        
        (
        w
        −
        a
        )
        +
        
          a
          
            2
          
        
        (
        w
        −
        a
        
          )
          
            2
          
        
        +
        ⋯
        ,
      
    
    {\displaystyle F_{0}(w)=h\circ f(w)=(w-a)^{-1}+a_{1}(w-a)+a_{2}(w-a)^{2}+\cdots ,}

with its image a horizontal slit domain. Suppose that 
 
 
 
 
 F
 
 1
 
 
 (
 w
 )
 
 
 {\displaystyle F_{1}(w)}
 
 is another uniformizer with

F
          
            1
          
        
        (
        w
        )
        =
        (
        w
        −
        a
        
          )
          
            −
            1
          
        
        +
        
          b
          
            1
          
        
        (
        w
        −
        a
        )
        +
        
          b
          
            2
          
        
        (
        w
        −
        a
        
          )
          
            2
          
        
        +
        ⋯
        .
      
    
    {\displaystyle F_{1}(w)=(w-a)^{-1}+b_{1}(w-a)+b_{2}(w-a)^{2}+\cdots .}

The images under 
 
 
 
 
 F
 
 0
 
 
 
 
 {\displaystyle F_{0}}
 
 or 
 
 
 
 
 F
 
 1
 
 
 
 
 {\displaystyle F_{1}}
 
 of each 
 
 
 
 
 C
 
 i
 
 
 
 
 {\displaystyle C_{i}}
 
 have a fixed y-coordinate so are horizontal segments. On the other hand, 
 
 
 
 
 F
 
 2
 
 
 (
 w
 )
 =
 
 F
 
 0
 
 
 (
 w
 )
 −
 
 F
 
 1
 
 
 (
 w
 )
 
 
 {\displaystyle F_{2}(w)=F_{0}(w)-F_{1}(w)}
 
 is holomorphic in 
 
 
 
 G
 
 
 {\displaystyle G}
 
. If it is constant, then it must be identically zero since 
 
 
 
 
 F
 
 2
 
 
 (
 a
 )
 =
 0
 
 
 {\displaystyle F_{2}(a)=0}
 
. Suppose 
 
 
 
 
 F
 
 2
 
 
 
 
 {\displaystyle F_{2}}
 
 is non-constant, then by assumption 
 
 
 
 
 F
 
 2
 
 
 (
 
 C
 
 i
 
 
 )
 
 
 {\displaystyle F_{2}(C_{i})}
 
 are all horizontal lines. If 
 
 
 
 t
 
 
 {\displaystyle t}
 
 is not in one of these lines, <a href="/facts/Cauchy%27s_argument_principle/TVJVoa2I">Cauchy's argument principle</a> shows that the number of solutions of 
 
 
 
 
 F
 
 2
 
 
 (
 w
 )
 =
 t
 
 
 {\displaystyle F_{2}(w)=t}
 
 in 
 
 
 
 G
 
 
 {\displaystyle G}
 
 is zero (any 
 
 
 
 t
 
 
 {\displaystyle t}
 
 will eventually be encircled by contours in 
 
 
 
 G
 
 
 {\displaystyle G}
 
 close to the 
 
 
 
 
 C
 
 i
 
 
 
 
 {\displaystyle C_{i}}
 
's). This contradicts the fact that the non-constant holomorphic function 
 
 
 
 
 F
 
 2
 
 
 
 
 {\displaystyle F_{2}}
 
 is an <a href="/facts/Open_mapping/abHUKX7l">open mapping</a>.<a class="footnote-ref" id="fnref:35" href="#fn:35">35</a>

<h2 id="sketch-proof-via-dirichlet-problem">Sketch proof via Dirichlet problem</h2>
Given 
 
 
 
 U
 
 
 {\displaystyle U}
 
 and a point 
 
 
 
 
 z
 
 0
 
 
 ∈
 U
 
 
 {\displaystyle z_{0}\in U}
 
, we want to construct a function 
 
 
 
 f
 
 
 {\displaystyle f}
 
 which maps 
 
 
 
 U
 
 
 {\displaystyle U}
 
 to the unit disk and 
 
 
 
 
 z
 
 0
 
 
 
 
 {\displaystyle z_{0}}
 
 to 
 
 
 
 0
 
 
 {\displaystyle 0}
 
. For this sketch, we will assume that U is bounded and its boundary is smooth, much like Riemann did. Write

f
        (
        z
        )
        =
        (
        z
        −
        
          z
          
            0
          
        
        )
        
          e
          
            g
            (
            z
            )
          
        
        ,
      
    
    {\displaystyle f(z)=(z-z_{0})e^{g(z)},}

where 
 
 
 
 g
 =
 u
 +
 i
 v
 
 
 {\displaystyle g=u+iv}
 
 is some (to be determined) holomorphic function with real part 
 
 
 
 u
 
 
 {\displaystyle u}
 
 and imaginary part 
 
 
 
 v
 
 
 {\displaystyle v}
 
. It is then clear that 
 
 
 
 
 z
 
 0
 
 
 
 
 {\displaystyle z_{0}}
 
 is the only zero of 
 
 
 
 f
 
 
 {\displaystyle f}
 
. We require 
 
 
 
 
 |
 
 f
 (
 z
 )
 
 |
 
 =
 1
 
 
 {\displaystyle |f(z)|=1}
 
 for 
 
 
 
 z
 ∈
 ∂
 U
 
 
 {\displaystyle z\in \partial U}
 
, so we need

u
        (
        z
        )
        =
        −
        log
        ⁡
        
          |
        
        z
        −
        
          z
          
            0
          
        
        
          |
        
      
    
    {\displaystyle u(z)=-\log |z-z_{0}|}

on the boundary. Since 
 
 
 
 u
 
 
 {\displaystyle u}
 
 is the real part of a holomorphic function, we know that 
 
 
 
 u
 
 
 {\displaystyle u}
 
 is necessarily a <a href="/facts/Harmonic_function/H6pg4dMT">harmonic function</a>; i.e., it satisfies <a href="/facts/Laplace%27s_equation/8n1YkmFS">Laplace's equation</a>.
The question then becomes: does a real-valued harmonic function 
 
 
 
 u
 
 
 {\displaystyle u}
 
 exist that is defined on all of 
 
 
 
 U
 
 
 {\displaystyle U}
 
 and has the given boundary condition? The positive answer is provided by the <a href="/facts/Dirichlet_principle/2PUtzTL8">Dirichlet principle</a>. Once the existence of 
 
 
 
 u
 
 
 {\displaystyle u}
 
 has been established, the <a href="/facts/Cauchy%E2%80%93Riemann_equations/SWkIHflU">Cauchy–Riemann equations</a> for the holomorphic function 
 
 
 
 g
 
 
 {\displaystyle g}
 
 allow us to find 
 
 
 
 v
 
 
 {\displaystyle v}
 
 (this argument depends on the assumption that 
 
 
 
 U
 
 
 {\displaystyle U}
 
 be simply connected). Once 
 
 
 
 u
 
 
 {\displaystyle u}
 
 and 
 
 
 
 v
 
 
 {\displaystyle v}
 
 have been constructed, one has to check that the resulting function 
 
 
 
 f
 
 
 {\displaystyle f}
 
 does indeed have all the required properties.<a class="footnote-ref" id="fnref:36" href="#fn:36">36</a>

<h2 id="uniformization-theorem">Uniformization theorem</h2>
The Riemann mapping theorem can be generalized to the context of <a href="/facts/Riemann_surface/qoj8ogv8">Riemann surfaces</a>: If 
 
 
 
 U
 
 
 {\displaystyle U}
 
 is a non-empty simply-connected open subset of a <a href="/facts/Riemann_surface/qoj8ogv8">Riemann surface</a>, then 
 
 
 
 U
 
 
 {\displaystyle U}
 
 is biholomorphic to one of the following: the <a href="/facts/Riemann_sphere/4XgBzplC">Riemann sphere</a>, the <a href="/facts/Complex_plane/vE0QrxJp">complex plane</a> 
 
 
 
 
 C
 
 
 
 {\displaystyle \mathbb {C} }
 
, or the <a href="/facts/Open_unit_disk/phrUu7yC">unit disk</a> 
 
 
 
 D
 
 
 {\displaystyle D}
 
. This is known as the <a href="/facts/Uniformization_theorem/mEa8a6IQ">uniformization theorem</a>.

<h2 id="smooth-riemann-mapping-theorem">Smooth Riemann mapping theorem</h2>
In the case of a simply connected bounded domain with smooth boundary, the Riemann mapping function and all its derivatives extend by continuity to the closure of the domain. This can be proved using regularity properties of solutions of the Dirichlet boundary value problem, which follow either from the theory of <a href="/facts/Sobolev_spaces_for_planar_domains/KRKImAoh">Sobolev spaces for planar domains</a> or from <a href="/facts/Neumann%E2%80%93Poincar%C3%A9_operator/3oDjNnFG">classical potential theory</a>. Other methods for proving the smooth Riemann mapping theorem include the theory of kernel functions<a class="footnote-ref" id="fnref:37" href="#fn:37">37</a> or the <a href="/facts/Beltrami_equation/vHofICHU">Beltrami equation</a>.

<h2 id="algorithms">Algorithms</h2>
Computational conformal mapping is prominently featured in problems of applied analysis and mathematical physics, as well as in engineering disciplines, such as image processing.
In the early 1980s an elementary algorithm for computing conformal maps was discovered. Given points 
 
 
 
 
 z
 
 0
 
 
 ,
 …
 ,
 
 z
 
 n
 
 
 
 
 {\displaystyle z_{0},\ldots ,z_{n}}
 
 in the plane, the algorithm computes an explicit conformal map of the unit disk onto a region bounded by a Jordan curve 
 
 
 
 γ
 
 
 {\displaystyle \gamma }
 
 with 
 
 
 
 
 z
 
 0
 
 
 ,
 …
 ,
 
 z
 
 n
 
 
 ∈
 γ
 .
 
 
 {\displaystyle z_{0},\ldots ,z_{n}\in \gamma .}
 
 This algorithm converges for Jordan regions<a class="footnote-ref" id="fnref:38" href="#fn:38">38</a> in the sense of uniformly close boundaries. There are corresponding uniform estimates on the closed region and the closed disc for the mapping functions and their inverses. Improved estimates are obtained if the data points lie on a 
 
 
 
 
 C
 
 1
 
 
 
 
 {\displaystyle C^{1}}
 
 curve or a K-<a href="/facts/Quasicircle/toHYYBmV">quasicircle</a>. The algorithm was discovered as an approximate method for conformal welding; however, it can also be viewed as a discretization of the <a href="/facts/Loewner_differential_equation/zWsYnBu8">Loewner differential equation</a>.<a class="footnote-ref" id="fnref:39" href="#fn:39">39</a>
The following is known about numerically approximating the conformal mapping between two planar domains.<a class="footnote-ref" id="fnref:40" href="#fn:40">40</a>
Positive results:

<ul><li>There is an algorithm A that computes the uniformizing map in the following sense. Let 
 
 
 
 Ω
 
 
 {\displaystyle \Omega }
 
 be a bounded simply-connected domain, and 
 
 
 
 
 w
 
 0
 
 
 ∈
 Ω
 
 
 {\displaystyle w_{0}\in \Omega }
 
. 
 
 
 
 ∂
 Ω
 
 
 {\displaystyle \partial \Omega }
 
 is provided to A by an oracle representing it in a pixelated sense (i.e., if the screen is divided to 
 
 
 
 
 2
 
 n
 
 
 ×
 
 2
 
 n
 
 
 
 
 {\displaystyle 2^{n}\times 2^{n}}
 
 pixels, the oracle can say whether each pixel belongs to the boundary or not). Then A computes the absolute values of the uniformizing map 
 
 
 
 ϕ
 :
 (
 Ω
 ,
 
 w
 
 0
 
 
 )
 →
 (
 D
 ,
 0
 )
 
 
 {\displaystyle \phi :(\Omega ,w_{0})\to (D,0)}
 
 with precision 
 
 
 
 
 2
 
 −
 n
 
 
 
 
 {\displaystyle 2^{-n}}
 
 in space bounded by 
 
 
 
 C
 
 n
 
 2
 
 
 
 
 {\displaystyle Cn^{2}}
 
 and time 
 
 
 
 
 2
 
 O
 (
 n
 )
 
 
 
 
 {\displaystyle 2^{O(n)}}
 
, where 
 
 
 
 C
 
 
 {\displaystyle C}
 
 depends only on the diameter of 
 
 
 
 Ω
 
 
 {\displaystyle \Omega }
 
 and 
 
 
 
 d
 (
 
 w
 
 0
 
 
 ,
 ∂
 Ω
 )
 .
 
 
 {\displaystyle d(w_{0},\partial \Omega ).}
 
 Furthermore, the algorithm computes the value of 
 
 
 
 ϕ
 (
 w
 )
 
 
 {\displaystyle \phi (w)}
 
 with precision 
 
 
 
 
 2
 
 −
 n
 
 
 
 
 {\displaystyle 2^{-n}}
 
 as long as 
 
 
 
 
 |
 
 ϕ
 (
 w
 )
 
 |
 
 <
 1
 −
 
 2
 
 −
 n
 
 
 .
 
 
 {\displaystyle |\phi (w)|<1-2^{-n}.}
 
 Moreover, A queries 
 
 
 
 ∂
 Ω
 
 
 {\displaystyle \partial \Omega }
 
 with precision of at most 
 
 
 
 
 2
 
 −
 O
 (
 n
 )
 
 
 .
 
 
 {\displaystyle 2^{-O(n)}.}
 
 In particular, if 
 
 
 
 ∂
 Ω
 
 
 {\displaystyle \partial \Omega }
 
 is polynomial space computable in space 
 
 
 
 
 n
 
 a
 
 
 
 
 {\displaystyle n^{a}}
 
 for some constant 
 
 
 
 a
 ≥
 1
 
 
 {\displaystyle a\geq 1}
 
 and time 
 
 
 
 T
 (
 n
 )
 <
 
 2
 
 O
 (
 
 n
 
 a
 
 
 )
 
 
 ,
 
 
 {\displaystyle T(n)<2^{O(n^{a})},}
 
 then A can be used to compute the uniformizing map in space 
 
 
 
 C
 ⋅
 
 n
 
 max
 (
 a
 ,
 2
 )
 
 
 
 
 {\displaystyle C\cdot n^{\max(a,2)}}
 
 and time 
 
 
 
 
 2
 
 O
 (
 
 n
 
 a
 
 
 )
 
 
 .
 
 
 {\displaystyle 2^{O(n^{a})}.}
 
</li></ul>
<ul><li>There is an algorithm A′ that computes the uniformizing map in the following sense. Let 
 
 
 
 Ω
 
 
 {\displaystyle \Omega }
 
 be a bounded simply-connected domain, and 
 
 
 
 
 w
 
 0
 
 
 ∈
 Ω
 .
 
 
 {\displaystyle w_{0}\in \Omega .}
 
 Suppose that for some 
 
 
 
 n
 =
 
 2
 
 k
 
 
 ,
 
 
 {\displaystyle n=2^{k},}
 
 
 
 
 
 ∂
 Ω
 
 
 {\displaystyle \partial \Omega }
 
 is given to A′ with precision 
 
 
 
 
 
 
 1
 n
 
 
 
 
 
 {\displaystyle {\tfrac {1}{n}}}
 
 by 
 
 
 
 O
 (
 
 n
 
 2
 
 
 )
 
 
 {\displaystyle O(n^{2})}
 
 pixels. Then A′ computes the absolute values of the uniformizing map 
 
 
 
 ϕ
 :
 (
 Ω
 ,
 
 w
 
 0
 
 
 )
 →
 (
 D
 ,
 0
 )
 
 
 {\displaystyle \phi :(\Omega ,w_{0})\to (D,0)}
 
 within an error of 
 
 
 
 O
 (
 1
 
 /
 
 n
 )
 
 
 {\displaystyle O(1/n)}
 
 in randomized space bounded by 
 
 
 
 O
 (
 k
 )
 
 
 {\displaystyle O(k)}
 
 and time polynomial in 
 
 
 
 n
 =
 
 2
 
 k
 
 
 
 
 {\displaystyle n=2^{k}}
 
 (that is, by a BPL(n)-machine). Furthermore, the algorithm computes the value of 
 
 
 
 ϕ
 (
 w
 )
 
 
 {\displaystyle \phi (w)}
 
 with precision 
 
 
 
 
 
 
 1
 n
 
 
 
 
 
 {\displaystyle {\tfrac {1}{n}}}
 
 as long as 
 
 
 
 
 |
 
 ϕ
 (
 w
 )
 
 |
 
 <
 1
 −
 
 
 
 1
 n
 
 
 
 .
 
 
 {\displaystyle |\phi (w)|<1-{\tfrac {1}{n}}.}
 
</li></ul>
Negative results:

<ul><li>Suppose there is an algorithm A that given a simply-connected domain 
 
 
 
 Ω
 
 
 {\displaystyle \Omega }
 
 with a linear-time computable boundary and an inner radius 
 
 
 
 >
 1
 
 /
 
 2
 
 
 {\displaystyle >1/2}
 
 and a number 
 
 
 
 n
 
 
 {\displaystyle n}
 
 computes the first 
 
 
 
 20
 n
 
 
 {\displaystyle 20n}
 
 digits of the <a href="/facts/Conformal_radius/LTc0horh">conformal radius</a> 
 
 
 
 r
 (
 Ω
 ,
 0
 )
 ,
 
 
 {\displaystyle r(\Omega ,0),}
 
 then we can use one call to A to solve any instance of a <a href="/facts/Sharp-SAT/AX8r9cBA">#SAT</a>(n) with a linear time overhead. In other words, <a href="/facts/Sharp-P/tY95TU7t">#P</a> is poly-time reducible to computing the conformal radius of a set.</li></ul>
<ul><li>Consider the problem of computing the conformal radius of a simply-connected domain 
 
 
 
 Ω
 ,
 
 
 {\displaystyle \Omega ,}
 
 where the boundary of 
 
 
 
 Ω
 
 
 {\displaystyle \Omega }
 
 is given with precision 
 
 
 
 1
 
 /
 
 n
 
 
 {\displaystyle 1/n}
 
 by an explicit collection of 
 
 
 
 O
 (
 
 n
 
 2
 
 
 )
 
 
 {\displaystyle O(n^{2})}
 
 pixels. Denote the problem of computing the conformal radius with precision 
 
 
 
 1
 
 /
 
 
 n
 
 c
 
 
 
 
 {\displaystyle 1/n^{c}}
 
 by 
 
 
 
 
 
 CONF
 
 
 (
 n
 ,
 
 n
 
 c
 
 
 )
 .
 
 
 {\displaystyle {\texttt {CONF}}(n,n^{c}).}
 
 Then, 
 
 
 
 
 
 
 MAJ
 
 
 
 n
 
 
 
 
 {\displaystyle {\texttt {MAJ}}_{n}}
 
 is <a href="/facts/AC0/UGJ79CeY">AC0</a> reducible to 
 
 
 
 
 
 CONF
 
 
 (
 n
 ,
 
 n
 
 c
 
 
 )
 
 
 {\displaystyle {\texttt {CONF}}(n,n^{c})}
 
 for any 
 
 
 
 0
 <
 c
 <
 
 
 
 1
 2
 
 
 
 .
 
 
 {\displaystyle 0<c<{\tfrac {1}{2}}.}
 
</li></ul>
<h2 id="see-also">See also</h2>
<ul><li><a href="/facts/Measurable_Riemann_mapping_theorem/DP0HQI8u">Measurable Riemann mapping theorem</a></li>
<li><a href="/facts/Schwarz%E2%80%93Christoffel_mapping/vzHbRDDG">Schwarz–Christoffel mapping</a> – a conformal transformation of the upper half-plane onto the interior of a simple polygon.</li>
<li><a href="/facts/Conformal_radius/LTc0horh">Conformal radius</a></li></ul>
<h2 id="notes">Notes</h2>

Wikimedia Commons has media related to Riemann mapping.

<ul><li><a href="/facts/Lars_Ahlfors/aukXlC2t">Ahlfors, Lars V.</a> (1978), Complex analysis. An introduction to the theory of analytic functions of one complex variable, International Series in Pure and Applied Mathematics (3rd ed.), McGraw-Hill, <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 0070006571</li>
<li><a href="/facts/Alan_Frank_Beardon/7j8kUweA">Beardon, Alan F.</a> (1979), Complex analysis.The argument principle in analysis and topology, John Wiley & Sons, <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 0471996718</li>
<li>Bell, Steven R. (1992), The Cauchy transform, potential theory, and conformal mapping, Studies in Advanced Mathematics, CRC Press, <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 0-8493-8270-X</li>
<li>Berenstein, Carlos A.; Gay, Roger (1991), Complex variables. An introduction, Graduate Texts in Mathematics, vol. 125, <a href="/facts/Springer-Verlag/nAesf6nT">Springer-Verlag</a>, <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 0387973494</li>
<li>Carathéodory, C. (1912), <a href="https://zenodo.org/record/1428282">"Untersuchungen über die konformen Abbildungen von festen und veranderlichen Gebieten"</a>, Mathematische Annalen, 72: 107–144, <a href="/facts/Doi_(identifier)/muM9Etpq">doi</a>:<a href="https://doi.org/10.1007%2Fbf01456892">10.1007/bf01456892</a>, <a href="/facts/S2CID_(identifier)/ldJsHa2Y">S2CID</a> <a href="https://api.semanticscholar.org/CorpusID:115544426">115544426</a></li>
<li><a href="/facts/John_B._Conway/7aMjnAxr">Conway, John B.</a> (1978), Functions of one complex variable, <a href="/facts/Springer-Verlag/nAesf6nT">Springer-Verlag</a>, <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 0-387-90328-3</li>
<li><a href="/facts/John_B._Conway/7aMjnAxr">Conway, John B.</a> (1995), Functions of one complex variable II, <a href="/facts/Springer-Verlag/nAesf6nT">Springer-Verlag</a>, <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 0-387-94460-5</li>
<li><a href="/facts/Peter_Duren/had6hlV6">Duren, P. L.</a> (1980), "Extremal problems for univalent functions", in Brannan, D.A.; Clunie, J.G. (eds.), Aspects of contemporary complex analysis, Academic Press, pp. 181–208, <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 9780121259501</li>
<li><a href="/facts/Peter_Duren/had6hlV6">Duren, P. L.</a> (1983), Univalent functions, Grundlehren der Mathematischen Wissenschaften, vol. 259, Springer-Verlag, <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 0-387-90795-5</li>
<li><a href="/facts/Theodore_Gamelin/6DbmKh36">Gamelin, Theodore W.</a> (2001), Complex analysis, Undergraduate Texts in Mathematics, Springer, <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 0-387-95069-9</li>
<li>Goluzin, G. M. (1969), Geometric theory of functions of a complex variable, Translations of Mathematical Monographs, vol. 26, American Mathematical Society</li>
<li><a href="/facts/Jeremy_Gray/Vbo8J5mk">Gray, Jeremy</a> (1994), <a href="http://www.math.stonybrook.edu/~bishop/classes/math401.F09/GrayRMT.pdf">"On the history of the Riemann mapping theorem"</a> (PDF), Rendiconti del Circolo Matematico di Palermo. Serie II. Supplemento (34): 47–94, <a href="/facts/MR_(identifier)/uP137L11">MR</a> <a href="https://mathscinet.ams.org/mathscinet-getitem?mr=1295591">1295591</a></li>
<li><a href="/facts/Robert_Everist_Greene/5QNAPDJB">Greene, Robert E.</a>; <a href="/facts/Kang-Tae_Kim/uAIXhzyS">Kim, Kang‑Tae</a> (2017), "The Riemann mapping theorem from Riemann's viewpoint", Complex Analysis and Its Synergies, 3, <a href="/facts/ArXiv_(identifier)/H6EtgnBe">arXiv</a>:<a href="https://arxiv.org/abs/1604.04071">1604.04071</a>, <a href="/facts/Doi_(identifier)/muM9Etpq">doi</a>:<a href="https://doi.org/10.1186%2Fs40627-016-0009-7">10.1186/s40627-016-0009-7</a></li>
<li><a href="/facts/Herbert_Gr%C3%B6tzsch/aDQtE0hR">Grötzsch, Herbert</a> (1932), "Über das Parallelschlitztheorem der konformen Abbildung schlichter Bereiche", Berichte über die Verhandlungen der Sächsischen Akademie der Wissenschaften zu Leipzig, Mathematisch-Physische Klasse (in German), 84: 15–36, <a href="/facts/Zbl_(identifier)/P6rFxKKx">Zbl</a> <a href="https://zbmath.org/?format=complete&q=an:0005.06802">0005.06802</a></li>
<li>Grunsky, Helmut (1978), Lectures on theory of functions in multiply connected domains, Studia Mathematica, vol. 4, Vandenhoeck & Ruprecht, <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-3-525-40142-2</li>
<li>Jänich, Klaus (1993), Funktionentheorie. Eine Einführung, Springer-Lehrbuch (in German) (3rd ed.), <a href="/facts/Springer-Verlag/nAesf6nT">Springer-Verlag</a>, <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 3540563377</li>
<li>Jenkins, James A. (1958), Univalent functions and conformal mapping., Ergebnisse der Mathematik und ihrer Grenzgebiete, vol. 18, <a href="/facts/Springer-Verlag/nAesf6nT">Springer-Verlag</a></li>
<li><a href="/facts/Kunihiko_Kodaira/u73B5W0D">Kodaira, Kunihiko</a> (2007), Complex analysis, Cambridge Studies in Advanced Mathematics, vol. 107, Cambridge University Press, <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 9780521809375</li>
<li><a href="/facts/Steven_G._Krantz/GkUkkFTA">Krantz, Steven G.</a> (2006), "Riemann Mapping Theorem and its Generalizations", Geometric Function Theory, <a href="/facts/Birkh%C3%A4user/brvgnrnJ">Birkhäuser</a>, pp. 83–108, <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 0-8176-4339-7</li>
<li><a href="/facts/Akhlesh_Lakhtakia/sNtb1HN9">Lakhtakia, Akhlesh</a>; Varadan, Vijay K.; Messier, Russell; <a href="/facts/Vasundara_Varadan/uYeUAzPr">Varadan, Vasundara</a> (1987), "Generalisations and randomisation of the plane Koch curve", Journal of Physics A: Mathematical and General, 20 (11): 3537–3541, <a href="/facts/Doi_(identifier)/muM9Etpq">doi</a>:<a href="https://doi.org/10.1088%2F0305-4470%2F20%2F11%2F052">10.1088/0305-4470/20/11/052</a></li>
<li><a href="/facts/Zeev_Nehari/Sc3fMc4k">Nehari, Zeev</a> (1952), Conformal mapping, <a href="/facts/Dover_Publications/RwjvlSFv">Dover Publications</a>, <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 9780486611372</li>
<li><a href="/facts/W._F._Osgood/1mTufCMj">Osgood, W. F.</a> (1900), "On the Existence of the Green's Function for the Most General Simply Connected Plane Region", <a href="/facts/Transactions_of_the_American_Mathematical_Society/JmKtyCwK">Transactions of the American Mathematical Society</a>, 1 (3), Providence, R.I.: <a href="/facts/American_Mathematical_Society/fr5gotCt">American Mathematical Society</a>: 310–314, <a href="/facts/Doi_(identifier)/muM9Etpq">doi</a>:<a href="https://doi.org/10.2307%2F1986285">10.2307/1986285</a>, <a href="/facts/ISSN_(identifier)/DPAflDvU">ISSN</a> <a href="https://search.worldcat.org/issn/0002-9947">0002-9947</a>, <a href="/facts/JFM_(identifier)/P6rFxKKx">JFM</a> <a href="https://zbmath.org/?format=complete&q=an:31.0420.01">31.0420.01</a>, <a href="/facts/JSTOR_(identifier)/YTeVmaJ7">JSTOR</a> <a href="https://www.jstor.org/stable/1986285">1986285</a></li>
<li><a href="/facts/Ren%C3%A9_de_Possel/IWCjBzFx">de Possel, René</a> (1931), <a href="https://gdz.sub.uni-goettingen.de/id/PPN252457811_1931?tify={%22pages%22:%5b203%5d,%22panX%22:0.758,%22panY%22:0.57,%22view%22:%22export%22,%22zoom%22:0.501}">"Zum Parallelschlitztheorm unendlich- vielfach zusammenhängender Gebiete"</a>, Nachrichten von der Gesellschaft der Wissenschaften zu Göttingen, Mathematisch-Physikalische Klasse (in German): 199−202</li>
<li><a href="/facts/Reinhold_Remmert/0rC0NDxz">Remmert, Reinhold</a> (1998), Classical topics in complex function theory, translated by <a href="/facts/Leslie_M._Kay/sjDtsg5v">Leslie M. Kay</a>, <a href="/facts/Springer-Verlag/nAesf6nT">Springer-Verlag</a>, <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 0-387-98221-3</li>
<li><a href="/facts/Bernhard_Riemann/oV2fL0k8">Riemann, Bernhard</a> (1851), <a href="http://www.emis.de/classics/Riemann/Grund.pdf">Grundlagen für eine allgemeine Theorie der Functionen einer veränderlichen complexen Grösse</a> (PDF) (in German), Göttingen{{citation}}: CS1 maint: location missing publisher (link)</li>
<li>Schiff, Joel L. (1993), Normal families, Universitext, <a href="/facts/Springer-Verlag/nAesf6nT">Springer-Verlag</a>, <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 0387979670</li>
<li>Schober, Glenn (1975), "Appendix C. Schiffer's boundary variation and fundamental lemma", Univalent functions—selected topics, Lecture Notes in Mathematics, vol. 478, <a href="/facts/Springer-Verlag/nAesf6nT">Springer-Verlag</a>, pp. 181–190</li>
<li><a href="/facts/Joseph_L._Walsh/eGYN1jk5">Walsh, J. L.</a> (1973), "History of the Riemann mapping theorem", <a href="/facts/American_Mathematical_Monthly/Te6CHvkg">The American Mathematical Monthly</a>, 80 (3): 270–276, <a href="/facts/Doi_(identifier)/muM9Etpq">doi</a>:<a href="https://doi.org/10.2307%2F2318448">10.2307/2318448</a>, <a href="/facts/ISSN_(identifier)/DPAflDvU">ISSN</a> <a href="https://search.worldcat.org/issn/0002-9890">0002-9890</a>, <a href="/facts/JSTOR_(identifier)/YTeVmaJ7">JSTOR</a> <a href="https://www.jstor.org/stable/2318448">2318448</a>, <a href="/facts/MR_(identifier)/uP137L11">MR</a> <a href="https://mathscinet.ams.org/mathscinet-getitem?mr=0323996">0323996</a></li></ul>
<h2 id="external-links">External links</h2>
<ul><li>Dolzhenko, E.P. (2001) [1994], <a href="https://www.encyclopediaofmath.org/index.php?title=Riemann_theorem">"Riemann theorem"</a>, <a href="/facts/Encyclopedia_of_Mathematics/WC6mGtPm">Encyclopedia of Mathematics</a>, <a href="/facts/European_Mathematical_Society/B3h7b672">EMS Press</a></li></ul>

<h2 id="references">References</h2>

<ol>
<li id="fn:1">The existence of f is equivalent to the existence of a Green’s function. <a href="/wiki/Green%E2%80%99s_function" target="_blank">/wiki/Green%E2%80%99s_function</a> <a href="#fnref:1" class="footnote-back-ref">↩</a></li>
<li id="fn:2">Ahlfors, Lars (1953), L. Ahlfors; E. Calabi; M. Morse; L. Sario; D. Spencer (eds.), "Developments of the Theory of Conformal Mapping and Riemann Surfaces Through a Century", Contributions to the Theory of Riemann Surfaces: 3–4 <a href="/wiki/Lars_Ahlfors" target="_blank">/wiki/Lars_Ahlfors</a> <a href="#fnref:2" class="footnote-back-ref">↩</a></li>
<li id="fn:3">For the original paper, see Osgood 1900. For accounts of the history, see Walsh 1973, pp. 270–271; Gray 1994, pp. 64–65; Greene & Kim 2017, p. 4. Also see Carathéodory 1912, p. 108, footnote ** (acknowledging that Osgood 1900 had already proven the Riemann mapping theorem). - Osgood, W. F. (1900), "On the Existence of the Green's Function for the Most General Simply Connected Plane Region", Transactions of the American Mathematical Society, 1 (3), Providence, R.I.: American Mathematical Society: 310–314, doi:10.2307/1986285, ISSN 0002-9947, JFM 31.0420.01, JSTOR 1986285 <a href="https://doi.org/10.2307%2F1986285" target="_blank">https://doi.org/10.2307%2F1986285</a> <a href="#fnref:3" class="footnote-back-ref">↩</a></li>
<li id="fn:4">Gray 1994, pp. 78–80, citing Carathéodory 1912 - Gray, Jeremy (1994), "On the history of the Riemann mapping theorem" (PDF), Rendiconti del Circolo Matematico di Palermo. Serie II. Supplemento (34): 47–94, MR 1295591 <a href="http://www.math.stonybrook.edu/~bishop/classes/math401.F09/GrayRMT.pdf" target="_blank">http://www.math.stonybrook.edu/~bishop/classes/math401.F09/GrayRMT.pdf</a> <a href="#fnref:4" class="footnote-back-ref">↩</a></li>
<li id="fn:5">Greene & Kim 2017, p. 1 - Greene, Robert E.; Kim, Kang‑Tae (2017), "The Riemann mapping theorem from Riemann's viewpoint", Complex Analysis and Its Synergies, 3, arXiv:1604.04071, doi:10.1186/s40627-016-0009-7 <a href="https://arxiv.org/abs/1604.04071" target="_blank">https://arxiv.org/abs/1604.04071</a> <a href="#fnref:5" class="footnote-back-ref">↩</a></li>
<li id="fn:6">Gray 1994, pp. 80–83 - Gray, Jeremy (1994), "On the history of the Riemann mapping theorem" (PDF), Rendiconti del Circolo Matematico di Palermo. Serie II. Supplemento (34): 47–94, MR 1295591 <a href="http://www.math.stonybrook.edu/~bishop/classes/math401.F09/GrayRMT.pdf" target="_blank">http://www.math.stonybrook.edu/~bishop/classes/math401.F09/GrayRMT.pdf</a> <a href="#fnref:6" class="footnote-back-ref">↩</a></li>
<li id="fn:7">"What did Riemann Contribute to Mathematics? Geometry, Number Theory and Others". <a href="https://www.researchgate.net/publication/344401528" target="_blank">https://www.researchgate.net/publication/344401528</a> <a href="#fnref:7" class="footnote-back-ref">↩</a></li>
<li id="fn:8">Lakhtakia, Akhlesh; Varadan, Vijay K.; Messier, Russell (August 1987). "Generalisations and randomisation of the plane Koch curve". Journal of Physics A: Mathematical and General. 20 (11): 3537–3541. doi:10.1088/0305-4470/20/11/052. <a href="/wiki/Doi_(identifier)" target="_blank">/wiki/Doi_(identifier)</a> <a href="#fnref:8" class="footnote-back-ref">↩</a></li>
<li id="fn:9">Remmert 1998, section 8.3, p. 187 - Remmert, Reinhold (1998), Classical topics in complex function theory, translated by Leslie M. Kay, Springer-Verlag, ISBN 0-387-98221-3 <a href="#fnref:9" class="footnote-back-ref">↩</a></li>
<li id="fn:10">See
Ahlfors 1978
Beardon 1979
Conway 1978
Gamelin 2001
 - Ahlfors, Lars V. (1978), Complex analysis. An introduction to the theory of analytic functions of one complex variable, International Series in Pure and Applied Mathematics (3rd ed.), McGraw-Hill, ISBN 0070006571 <a href="#fnref:10" class="footnote-back-ref">↩</a></li>
<li id="fn:11">Gamelin 2001, pp. 256–257, elementary proof - Gamelin, Theodore W. (2001), Complex analysis, Undergraduate Texts in Mathematics, Springer, ISBN 0-387-95069-9 <a href="#fnref:11" class="footnote-back-ref">↩</a></li>
<li id="fn:12">Berenstein & Gay 1991, pp. 86–87 - Berenstein, Carlos A.; Gay, Roger (1991), Complex variables. An introduction, Graduate Texts in Mathematics, vol. 125, Springer-Verlag, ISBN 0387973494 <a href="#fnref:12" class="footnote-back-ref">↩</a></li>
<li id="fn:13">Gamelin 2001 - Gamelin, Theodore W. (2001), Complex analysis, Undergraduate Texts in Mathematics, Springer, ISBN 0-387-95069-9 <a href="#fnref:13" class="footnote-back-ref">↩</a></li>
<li id="fn:14">Gamelin 2001 - Gamelin, Theodore W. (2001), Complex analysis, Undergraduate Texts in Mathematics, Springer, ISBN 0-387-95069-9 <a href="#fnref:14" class="footnote-back-ref">↩</a></li>
<li id="fn:15">Duren 1983 - Duren, P. L. (1983), Univalent functions, Grundlehren der Mathematischen Wissenschaften, vol. 259, Springer-Verlag, ISBN 0-387-90795-5 <a href="#fnref:15" class="footnote-back-ref">↩</a></li>
<li id="fn:16">Jänich 1993 - Jänich, Klaus (1993), Funktionentheorie. Eine Einführung, Springer-Lehrbuch (in German) (3rd ed.), Springer-Verlag, ISBN 3540563377 <a href="#fnref:16" class="footnote-back-ref">↩</a></li>
<li id="fn:17">Duren 1983 - Duren, P. L. (1983), Univalent functions, Grundlehren der Mathematischen Wissenschaften, vol. 259, Springer-Verlag, ISBN 0-387-90795-5 <a href="#fnref:17" class="footnote-back-ref">↩</a></li>
<li id="fn:18">Jänich 1993 - Jänich, Klaus (1993), Funktionentheorie. Eine Einführung, Springer-Lehrbuch (in German) (3rd ed.), Springer-Verlag, ISBN 3540563377 <a href="#fnref:18" class="footnote-back-ref">↩</a></li>
<li id="fn:19">Gamelin 2001, p. 309 - Gamelin, Theodore W. (2001), Complex analysis, Undergraduate Texts in Mathematics, Springer, ISBN 0-387-95069-9 <a href="#fnref:19" class="footnote-back-ref">↩</a></li>
<li id="fn:20">Duren 1983 - Duren, P. L. (1983), Univalent functions, Grundlehren der Mathematischen Wissenschaften, vol. 259, Springer-Verlag, ISBN 0-387-90795-5 <a href="#fnref:20" class="footnote-back-ref">↩</a></li>
<li id="fn:21">Jänich 1993 - Jänich, Klaus (1993), Funktionentheorie. Eine Einführung, Springer-Lehrbuch (in German) (3rd ed.), Springer-Verlag, ISBN 3540563377 <a href="#fnref:21" class="footnote-back-ref">↩</a></li>
<li id="fn:22">Ahlfors 1978 - Ahlfors, Lars V. (1978), Complex analysis. An introduction to the theory of analytic functions of one complex variable, International Series in Pure and Applied Mathematics (3rd ed.), McGraw-Hill, ISBN 0070006571 <a href="#fnref:22" class="footnote-back-ref">↩</a></li>
<li id="fn:23">Jenkins 1958, pp. 77–78 - Jenkins, James A. (1958), Univalent functions and conformal mapping., Ergebnisse der Mathematik und ihrer Grenzgebiete, vol. 18, Springer-Verlag <a href="#fnref:23" class="footnote-back-ref">↩</a></li>
<li id="fn:24">Duren 1980 - Duren, P. L. (1980), "Extremal problems for univalent functions", in Brannan, D.A.; Clunie, J.G. (eds.), Aspects of contemporary complex analysis, Academic Press, pp. 181–208, ISBN 9780121259501 <a href="#fnref:24" class="footnote-back-ref">↩</a></li>
<li id="fn:25">Schiff 1993, pp. 162–166 - Schiff, Joel L. (1993), Normal families, Universitext, Springer-Verlag, ISBN 0387979670 <a href="#fnref:25" class="footnote-back-ref">↩</a></li>
<li id="fn:26">Jenkins 1958, pp. 77–78 - Jenkins, James A. (1958), Univalent functions and conformal mapping., Ergebnisse der Mathematik und ihrer Grenzgebiete, vol. 18, Springer-Verlag <a href="#fnref:26" class="footnote-back-ref">↩</a></li>
<li id="fn:27">Schober 1975 - Schober, Glenn (1975), "Appendix C. Schiffer's boundary variation and fundamental lemma", Univalent functions—selected topics, Lecture Notes in Mathematics, vol. 478, Springer-Verlag, pp. 181–190 <a href="#fnref:27" class="footnote-back-ref">↩</a></li>
<li id="fn:28">Duren 1980 - Duren, P. L. (1980), "Extremal problems for univalent functions", in Brannan, D.A.; Clunie, J.G. (eds.), Aspects of contemporary complex analysis, Academic Press, pp. 181–208, ISBN 9780121259501 <a href="#fnref:28" class="footnote-back-ref">↩</a></li>
<li id="fn:29">Duren 1983 - Duren, P. L. (1983), Univalent functions, Grundlehren der Mathematischen Wissenschaften, vol. 259, Springer-Verlag, ISBN 0-387-90795-5 <a href="#fnref:29" class="footnote-back-ref">↩</a></li>
<li id="fn:30">Schiff 1993 - Schiff, Joel L. (1993), Normal families, Universitext, Springer-Verlag, ISBN 0387979670 <a href="#fnref:30" class="footnote-back-ref">↩</a></li>
<li id="fn:31">Goluzin 1969, pp. 210–216 - Goluzin, G. M. (1969), Geometric theory of functions of a complex variable, Translations of Mathematical Monographs, vol. 26, American Mathematical Society <a href="#fnref:31" class="footnote-back-ref">↩</a></li>
<li id="fn:32">Schiff 1993 - Schiff, Joel L. (1993), Normal families, Universitext, Springer-Verlag, ISBN 0387979670 <a href="#fnref:32" class="footnote-back-ref">↩</a></li>
<li id="fn:33">Goluzin 1969, pp. 210–216 - Goluzin, G. M. (1969), Geometric theory of functions of a complex variable, Translations of Mathematical Monographs, vol. 26, American Mathematical Society <a href="#fnref:33" class="footnote-back-ref">↩</a></li>
<li id="fn:34">Nehari 1952, pp. 351–358 - Nehari, Zeev (1952), Conformal mapping, Dover Publications, ISBN 9780486611372 <a href="#fnref:34" class="footnote-back-ref">↩</a></li>
<li id="fn:35">Goluzin 1969, pp. 214−215 - Goluzin, G. M. (1969), Geometric theory of functions of a complex variable, Translations of Mathematical Monographs, vol. 26, American Mathematical Society <a href="#fnref:35" class="footnote-back-ref">↩</a></li>
<li id="fn:36">Gamelin 2001, pp. 390–407 - Gamelin, Theodore W. (2001), Complex analysis, Undergraduate Texts in Mathematics, Springer, ISBN 0-387-95069-9 <a href="#fnref:36" class="footnote-back-ref">↩</a></li>
<li id="fn:37">Bell 1992 - Bell, Steven R. (1992), The Cauchy transform, potential theory, and conformal mapping, Studies in Advanced Mathematics, CRC Press, ISBN 0-8493-8270-X <a href="#fnref:37" class="footnote-back-ref">↩</a></li>
<li id="fn:38">A Jordan region is the interior of a Jordan curve. <a href="/wiki/Jordan_curve" target="_blank">/wiki/Jordan_curve</a> <a href="#fnref:38" class="footnote-back-ref">↩</a></li>
<li id="fn:39">Marshall, Donald E.; Rohde, Steffen (2007). "Convergence of a Variant of the Zipper Algorithm for Conformal Mapping". SIAM Journal on Numerical Analysis. 45 (6): 2577. CiteSeerX 10.1.1.100.2423. doi:10.1137/060659119. <a href="/wiki/CiteSeerX_(identifier)" target="_blank">/wiki/CiteSeerX_(identifier)</a> <a href="#fnref:39" class="footnote-back-ref">↩</a></li>
<li id="fn:40">Binder, Ilia; Braverman, Mark; Yampolsky, Michael (2007). "On the computational complexity of the Riemann mapping". Arkiv för Matematik. 45 (2): 221. arXiv:math/0505617. Bibcode:2007ArM....45..221B. doi:10.1007/s11512-007-0045-x. S2CID 14545404. <a href="/wiki/ArXiv_(identifier)" target="_blank">/wiki/ArXiv_(identifier)</a> <a href="#fnref:40" class="footnote-back-ref">↩</a></li>
</ol>

Riemann mapping theorem open-in-new

Riemann mapping theorem