area theorem (conformal mapping)
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theory of
conformal mapping In mathematics, a conformal map is a function that locally preserves angles, but not necessarily lengths. More formally, let U and V be open subsets of \mathbb^n. A function f:U\to V is called conformal (or angle-preserving) at a point u_0\in ...
s, the area theorem gives an
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satisfied by the
power series In mathematics, a power series (in one variable) is an infinite series of the form \sum_^\infty a_n \left(x - c\right)^n = a_0 + a_1 (x - c) + a_2 (x - c)^2 + \dots where ''an'' represents the coefficient of the ''n''th term and ''c'' is a con ...
coefficients of certain conformal mappings. The theorem is called by that name, not because of its implications, but rather because the proof uses the notion of
area Area is the quantity that expresses the extent of a region on the plane or on a curved surface. The area of a plane region or ''plane area'' refers to the area of a shape or planar lamina, while '' surface area'' refers to the area of an ope ...
.


Statement

Suppose that f is analytic and injective in the punctured
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unit disk \mathbb D\setminus\ and has the power series representation : f(z)= \frac 1z + \sum_^\infty a_n z^n,\qquad z\in \mathbb D\setminus\, then the coefficients a_n satisfy : \sum_^\infty n, a_n, ^2\le 1.


Proof

The idea of the proof is to look at the area uncovered by the image of f. Define for r\in(0,1) :\gamma_r(\theta):=f(r\,e^),\qquad \theta\in ,2\pi Then \gamma_r is a simple closed curve in the plane. Let D_r denote the unique bounded connected component of \mathbb C\setminus\gamma_r( ,2\pi. The existence and uniqueness of D_r follows from Jordan's curve theorem. If D is a domain in the plane whose boundary is a
smooth Smooth may refer to: Mathematics * Smooth function, a function that is infinitely differentiable; used in calculus and topology * Smooth manifold, a differentiable manifold for which all the transition maps are smooth functions * Smooth algebrai ...
simple closed curve \gamma, then : \mathrm(D)=\int_\gamma x\,dy=-\int_\gamma y\,dx\,, provided that \gamma is positively oriented around D. This follows easily, for example, from Green's theorem. As we will soon see, \gamma_r is positively oriented around D_r (and that is the reason for the minus sign in the definition of \gamma_r). After applying the
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and the formula for \gamma_r, the above expressions for the area give : \mathrm(D_r)= \int_0^ \Re\bigl(f(r e^)\bigr)\,\Im\bigl(-i\,r\,e^\,f'(r e^)\bigr)\,d\theta = -\int_0^ \Im\bigl(f(r e^)\bigr)\,\Re\bigl(-i\,r\,e^\,f'(r e^)\bigr)d\theta. Therefore, the area of D_r also equals to the average of the two expressions on the right hand side. After simplification, this yields : \mathrm(D_r) = -\frac 12\, \Re\int_0^f(r\,e^)\,\overline\,d\theta, where \overline z denotes complex conjugation. We set a_=1 and use the power series expansion for f, to get : \mathrm(D_r) = -\frac 12\, \Re\int_0^ \sum_^\infty \sum_^\infty m\,r^\,a_n\,\overline\,e^\,d\theta\,. (Since \int_0^ \sum_^\infty\sum_^\infty m\,r^\,, a_n, \,, a_m, \,d\theta<\infty\,, the rearrangement of the terms is justified.) Now note that \int_0^ e^\,d\theta is 2\pi if n= m and is zero otherwise. Therefore, we get : \mathrm(D_r)= -\pi\sum_^\infty n\,r^\,, a_n, ^2. The area of D_r is clearly positive. Therefore, the right hand side is positive. Since a_=1, by letting r\to1, the theorem now follows. It only remains to justify the claim that \gamma_r is positively oriented around D_r. Let r' satisfy r, and set z_0=f(r'), say. For very small s>0, we may write the expression for the
winding number In mathematics, the winding number or winding index of a closed curve in the plane around a given point is an integer representing the total number of times that curve travels counterclockwise around the point, i.e., the curve's number of t ...
of \gamma_s around z_0, and verify that it is equal to 1. Since, \gamma_t does not pass through z_0 when t\ne r' (as f is injective), the invariance of the winding number under homotopy in the complement of z_0 implies that the winding number of \gamma_r around z_0 is also 1. This implies that z_0\in D_r and that \gamma_r is positively oriented around D_r, as required.


Uses

The inequalities satisfied by power series coefficients of conformal mappings were of considerable interest to mathematicians prior to the solution of the
Bieberbach conjecture In complex analysis, de Branges's theorem, or the Bieberbach conjecture, is a theorem that gives a necessary condition on a holomorphic function in order for it to map the open unit disk of the complex plane injectively to the complex plane. It ...
. The area theorem is a central tool in this context. Moreover, the area theorem is often used in order to prove the
Koebe 1/4 theorem In complex analysis, a branch of mathematics, the Koebe 1/4 theorem states the following: Koebe Quarter Theorem. The image of an injective analytic function f:\mathbf\to\mathbb from the unit disk \mathbf onto a subset of the complex plane con ...
, which is very useful in the study of the geometry of conformal mappings.


References

*{{Citation , last1=Rudin , first1=Walter , author1-link=Walter Rudin , title=Real and complex analysis , publisher=McGraw-Hill Book Co. , location=New York , edition=3rd , isbn=978-0-07-054234-1 , mr=924157 , year=1987 , oclc=13093736 Theorems in complex analysis Articles containing proofs