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== Riemann's theorem == [[Bernhard Riemann|Riemann's]] theorem on removable singularities is as follows: {{math theorem| Let <math>D \subset \mathbb C</math> be an open subset of the complex plane, <math>a \in D</math> a point of <math>D</math> and <math>f</math> a holomorphic function defined on the set <math>D \setminus \{a\}</math>. The following are equivalent: # <math>f</math> is holomorphically extendable over <math>a</math>. # <math>f</math> is continuously extendable over <math>a</math>. # There exists a [[neighborhood (topology)|neighborhood]] of <math>a</math> on which <math>f</math> is [[bounded function|bounded]]. # <math>\lim_{z\to a}(z - a) f(z) = 0</math>.}} The implications 1 β 2 β 3 β 4 are trivial. To prove 4 β 1, we first recall that the holomorphy of a function at <math>a</math> is equivalent to it being analytic at <math>a</math> ([[Proof that holomorphic functions are analytic|proof]]), i.e. having a power series representation. Define :<math> h(z) = \begin{cases} (z - a)^2 f(z) & z \ne a ,\\ 0 & z = a . \end{cases} </math> Clearly, ''h'' is holomorphic on <math> D \setminus \{a\}</math>, and there exists :<math>h'(a)=\lim_{z\to a}\frac{(z - a)^2f(z)-0}{z-a}=\lim_{z\to a}(z - a) f(z)=0</math> by 4, hence ''h'' is holomorphic on ''D'' and has a [[Taylor series]] about ''a'': :<math>h(z) = c_0 + c_1(z-a) + c_2 (z - a)^2 + c_3 (z - a)^3 + \cdots \, .</math> We have ''c''<sub>0</sub> = ''h''(''a'') = 0 and ''c''<sub>1</sub> = ''h{{'}}''(''a'') = 0; therefore :<math>h(z) = c_2 (z - a)^2 + c_3 (z - a)^3 + \cdots \, .</math> Hence, where <math>z \ne a</math>, we have: :<math>f(z) = \frac{h(z)}{(z - a)^2} = c_2 + c_3 (z - a) + \cdots \, .</math> However, :<math>g(z) = c_2 + c_3 (z - a) + \cdots \, .</math> is holomorphic on ''D'', thus an extension of <math> f </math>.
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