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Cauchy's integral theorem
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=== Fundamental theorem for complex line integrals === If {{math|''f''(''z'')}} is a holomorphic function on an open [[region (mathematical analysis)|region]] {{mvar|U}}, and <math>\gamma</math> is a curve in {{mvar|U}} from <math>z_0</math> to <math>z_1</math> then, <math display="block">\int_{\gamma}f'(z) \, dz = f(z_1)-f(z_0).</math> Also, when {{math|''f''(''z'')}} has a single-valued antiderivative in an open region {{mvar|U}}, then the path integral <math display="inline">\int_{\gamma}f(z) \, dz</math> is path independent for all paths in {{mvar|U}}. ==== Formulation on simply connected regions ==== Let <math>U \subseteq \Complex</math> be a [[Simply connected space|simply connected]] [[open subset|open]] set, and let <math>f: U \to \Complex</math> be a [[holomorphic function]]. Let <math>\gamma: [a,b] \to U</math> be a smooth closed curve. Then: <math display="block">\int_\gamma f(z)\,dz = 0. </math> (The condition that <math>U</math> be [[simply connected]] means that <math>U</math> has no "holes", or in other words, that the [[fundamental group]] of <math>U</math> is trivial.) ==== General formulation ==== Let <math>U \subseteq \Complex</math> be an [[open subset|open set]], and let <math>f: U \to \Complex</math> be a [[holomorphic function]]. Let <math>\gamma: [a,b] \to U</math> be a smooth closed curve. If <math>\gamma</math> is [[Homotopy|homotopic]] to a constant curve, then: <math display="block">\int_\gamma f(z)\,dz = 0. </math>where z Ρ ''U'' (Recall that a curve is [[Homotopy|homotopic]] to a constant curve if there exists a smooth [[homotopy]] (within <math>U</math>) from the curve to the constant curve. Intuitively, this means that one can shrink the curve into a point without exiting the space.) The first version is a special case of this because on a [[Simply connected space|simply connected]] set, every closed curve is [[Homotopy|homotopic]] to a constant curve. ==== Main example ==== In both cases, it is important to remember that the curve <math>\gamma</math> does not surround any "holes" in the domain, or else the theorem does not apply. A famous example is the following curve: <math display="block">\gamma(t) = e^{it} \quad t \in \left[0, 2\pi\right] ,</math> which traces out the unit circle. Here the following integral: <math display="block">\int_{\gamma} \frac{1}{z}\,dz = 2\pi i \neq 0 , </math> is nonzero. The Cauchy integral theorem does not apply here since <math>f(z) = 1/z</math> is not defined at <math>z = 0</math>. Intuitively, <math>\gamma</math> surrounds a "hole" in the domain of <math>f</math>, so <math>\gamma</math> cannot be shrunk to a point without exiting the space. Thus, the theorem does not apply.
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