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Complex Analysis - Maths KU

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D C<br />

Figure 5.26 Simply connected<br />

domain D<br />

C 1<br />

D<br />

C 2<br />

Figure 5.27 Multiply connected<br />

domain D<br />

Green’s theorem expresses a real<br />

line integral as a double integral<br />

☞<br />

5.3 Cauchy-Goursat Theorem 257<br />

D. Expressed yet another way, a simply connected domain has no “holes” in<br />

it. The entire complex plane is an example of a simply connected domain;<br />

the annulus defined by 1 < |z| < 2 is not simply connected. (Why?) A domain<br />

that is not simply connected is called a multiply connected domain;<br />

that is, a multiply connected domain has “holes” in it. Note in Figure 5.27<br />

that if the curve C2 enclosing the “hole” were shrunk to a point, the curve<br />

would have to leave D eventually. We call a domain with one “hole” doubly<br />

connected, a domain with two “holes” triply connected, and so on. The<br />

open disk defined by |z| < 2 is a simply connected domain; the open circular<br />

annulus defined by 1 < |z| < 2 is a doubly connected domain.<br />

Cauchy’s Theorem In 1825 the French mathematician Louis-Augustin<br />

Cauchy proved one the most important theorems in complex analysis.<br />

Cauchy’s Theorem<br />

Suppose that a function f is analytic in a simply connected domain<br />

D and that f ′ is continuous in D. Then for every simple closed (1)<br />

contour C in D, �<br />

f(z) dz =0.<br />

C<br />

Cauchy’s Proof of (1) The proof of this theorem is an immediate consequence<br />

of Green’s theoremin the plane and the Cauchy-Riemann equations.<br />

Recall fromcalculus that if C is a positively oriented, piecewise smooth, simple<br />

closed curve forming the boundary of a region R within D, and if the<br />

real-valued functions P (x, y) and Q(x, y) along with their first-order partial<br />

derivatives are continuous on a domain that contains C and R, then<br />

�<br />

C<br />

�� � �<br />

∂Q ∂P<br />

Pdx+ Qdy = − dA. (2)<br />

R ∂x ∂y<br />

Now in the statement (1) we have assumed that f ′ is continuous throughout<br />

the domain D. As a consequence, the real and imaginary parts of f(z) =u+iv<br />

and their first partial derivatives are continuous throughout D. By (9) of<br />

Section 5.2 we write �<br />

f(z) dz in terms of real line integrals and apply Green’s<br />

C<br />

theorem(2) to each line integral:<br />

�<br />

C<br />

�<br />

�<br />

f(z) dz = u(x, y) dx − v(x, y) dy + i<br />

C<br />

��<br />

=<br />

�<br />

− ∂v<br />

� ��<br />

∂u<br />

− dA + i<br />

∂x ∂y<br />

R<br />

C<br />

R<br />

v(x, y) dx + u(x, y) dy<br />

� �<br />

∂u ∂v<br />

− dA. (3)<br />

∂x ∂y<br />

Because f is analytic in D, the real functions u and v satisfy the Cauchy-<br />

Riemann equations, ∂u/∂x = ∂v/∂y and ∂u/∂y = −∂v/∂x, at every point in

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