TheoremComplete

Cauchy-Goursat Theorem

The Cauchy-Goursat theorem eliminates the need to assume continuity of f′f' in Cauchy's original theorem. This refinement, due to Goursat, shows that holomorphicity alone suffices to guarantee vanishing of contour integrals.


Statement of the Theorem

Theorem3.9Cauchy-Goursat theorem

Let ff be holomorphic on a simply connected domain DD. Then for every closed contour γ\gamma in DD:

∮γf(z) dz=0.\oint_\gamma f(z)\,dz = 0.

More precisely, if ff is holomorphic inside and on a simple closed contour γ\gamma, then ∮γf(z) dz=0\oint_\gamma f(z)\,dz = 0.

RemarkHistorical significance

Cauchy's original proof (1825) assumed that f′f' is continuous. Goursat (1900) showed this assumption is unnecessary: the mere existence of f′(z)f'(z) at each point suffices. This is a remarkable strengthening, as in real analysis, a differentiable function need not have a continuous derivative.


Proof Strategy

Proof

We prove the theorem for a triangle TT; the general case follows by triangulation.

Step 1. Subdivide TT into four congruent triangles T1,T2,T3,T4T_1, T_2, T_3, T_4 by connecting edge midpoints. Then

∮∂Tf dz=∑j=14∮∂Tjf dz\oint_{\partial T} f\,dz = \sum_{j=1}^4 \oint_{\partial T_j} f\,dz

since integrals over shared interior edges cancel (traversed in opposite directions).

Step 2. Choose T(1)T^{(1)} among {Tj}\{T_j\} with ∣∮∂T(1)f dz∣≥14∣∮∂Tf dz∣\left|\oint_{\partial T^{(1)}} f\,dz\right| \geq \frac{1}{4}\left|\oint_{\partial T} f\,dz\right|.

Iterate to obtain a nested sequence T⊃T(1)⊃T(2)⊃⋯T \supset T^{(1)} \supset T^{(2)} \supset \cdots with diam(T(n))=2−ndiam(T)\text{diam}(T^{(n)}) = 2^{-n}\text{diam}(T), L(∂T(n))=2−nL(∂T)L(\partial T^{(n)}) = 2^{-n}L(\partial T), and

∣∮∂T(n)f dz∣≥4−n∣∮∂Tf dz∣.\left|\oint_{\partial T^{(n)}} f\,dz\right| \geq 4^{-n}\left|\oint_{\partial T} f\,dz\right|.

Step 3. By the nested intervals property, ⋂nT(n)={z0}\bigcap_n T^{(n)} = \{z_0\} for some z0∈Dz_0 \in D. Since ff is differentiable at z0z_0:

f(z)=f(z0)+f′(z0)(z−z0)+ε(z)(z−z0)f(z) = f(z_0) + f'(z_0)(z - z_0) + \varepsilon(z)(z - z_0)

where ε(z)→0\varepsilon(z) \to 0 as z→z0z \to z_0.

Step 4. The integral of f(z0)+f′(z0)(z−z0)f(z_0) + f'(z_0)(z-z_0) over any closed contour vanishes (it has an antiderivative). Therefore:

∣∮∂T(n)f dz∣=∣∮∂T(n)ε(z)(z−z0) dz∣≤sup⁡z∈T(n)∣ε(z)∣⋅diam(T(n))⋅L(∂T(n)).\left|\oint_{\partial T^{(n)}} f\,dz\right| = \left|\oint_{\partial T^{(n)}} \varepsilon(z)(z-z_0)\,dz\right| \leq \sup_{z \in T^{(n)}} |\varepsilon(z)| \cdot \text{diam}(T^{(n)}) \cdot L(\partial T^{(n)}).

This gives 4−n∣∮∂Tf dz∣≤sup⁡∣ε∣⋅4−ndiam(T)⋅L(∂T)4^{-n}\left|\oint_{\partial T} f\,dz\right| \leq \sup|\varepsilon| \cdot 4^{-n}\text{diam}(T) \cdot L(\partial T).

Since sup⁡∣ε∣→0\sup|\varepsilon| \to 0, we conclude ∮∂Tf dz=0\oint_{\partial T} f\,dz = 0. ■\blacksquare

■

Extensions and Generalizations

Theorem3.10Cauchy's theorem for multiply connected domains

If ff is holomorphic on a domain bounded by a positively oriented outer contour γ0\gamma_0 and negatively oriented inner contours γ1,…,γn\gamma_1, \ldots, \gamma_n, then

∮γ0f dz+∮γ1f dz+⋯+∮γnf dz=0.\oint_{\gamma_0} f\,dz + \oint_{\gamma_1} f\,dz + \cdots + \oint_{\gamma_n} f\,dz = 0.

Equivalently, ∮γ0f dz=∑k=1n∮γk+f dz\oint_{\gamma_0} f\,dz = \sum_{k=1}^n \oint_{\gamma_k^+} f\,dz where γk+\gamma_k^+ denotes positive orientation.

ExampleApplication to annular regions

Let f(z)=1/(z2+1)f(z) = 1/(z^2 + 1) and consider the annular region between ∣z∣=2|z| = 2 and ∣z−i∣=1/2|z - i| = 1/2. Since the only singularity inside ∣z∣=2|z| = 2 in the upper half-plane is z=iz = i:

∮∣z∣=2dzz2+1=∮∣z−i∣=1/2dzz2+1=∮∣z−i∣=1/21/(z+i)z−i dz=2πi⋅12i=π.\oint_{|z|=2} \frac{dz}{z^2+1} = \oint_{|z-i|=1/2} \frac{dz}{z^2+1} = \oint_{|z-i|=1/2} \frac{1/(z+i)}{z-i}\,dz = 2\pi i \cdot \frac{1}{2i} = \pi.

RemarkMorera's theorem — the converse

Morera's theorem provides a converse: if ff is continuous on a domain DD and ∮γf dz=0\oint_\gamma f\,dz = 0 for every closed triangle (or closed contour) in DD, then ff is holomorphic on DD. This is remarkably useful for proving holomorphicity of functions defined by integrals.