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removable singularity : ウィキペディア英語版
removable singularity

In complex analysis, a removable singularity of a holomorphic function is a point at which the function is undefined, but it is possible to define the function at that point in such a way that the function is regular in a neighbourhood of that point.
For instance, the (unnormalized) sinc function
: \text(z) = \frac
has a singularity at ''z'' = 0. This singularity can be removed by defining ''f''(0) := 1, which is the limit of ''f'' as ''z'' tends to 0. The resulting function is holomorphic. In this case the problem was caused by ''f'' being given an indeterminate form. Taking a power series expansion for \frac shows that
: \text(z) = \frac\left(\sum_^ \frac \right) = \sum_^ \frac = 1 - \frac + \frac - \frac + \cdots.
Formally, if U \subset \mathbb C is an open subset of the complex plane \mathbb C, a \in U a point of U, and f: U\setminus \ \rightarrow \mathbb C is a holomorphic function, then a is called a removable singularity for f if there exists a holomorphic function g: U \rightarrow \mathbb C which coincides with f on U\setminus \. We say f is holomorphically extendable over U if such a g exists.
== Riemann's theorem ==

Riemann's theorem on removable singularities states when a singularity is removable:
Theorem. Let D \subset C be an open subset of the complex plane, a \in D a point of D and f a holomorphic function defined on the set D \setminus \. The following are equivalent:
# f is holomorphically extendable over a.
# f is continuously extendable over a.
# There exists a neighborhood of a on which f is bounded.
# \lim_(z - a) f(z) = 0.
The implications 1 ⇒ 2 ⇒ 3 ⇒ 4 are trivial. To prove 4 ⇒ 1, we first recall that the holomorphy of a function at a is equivalent to it being analytic at a (proof), i.e. having a power series representation. Define
:
h(z) = \begin
(z - a)^2 f(z) & z \ne a ,\\
0 & z = a .
\end

Clearly, ''h'' is holomorphic on ''D'' \ , and there exists
:h'(a)=\lim_\frac=\lim_(z - a) f(z)=0
by 4, hence ''h'' is holomorphic on ''D'' and has a Taylor series about ''a'':
:h(z) = c_0 + c_1(z-a) + c_2 (z - a)^2 + c_3 (z - a)^3 + \cdots \, .
We have ''c''0 = ''h''(''a'') = 0 and ''c''1 = ''h''(''a'') = 0; therefore
:h(z) = c_2 (z - a)^2 + c_3 (z - a)^3 + \cdots \, .
Hence, where z≠a, we have:
:f(z) = \frac = c_2 + c_3 (z - a) + \cdots \, .
However,
:g(z) = c_2 + c_3 (z - a) + \cdots \, .
is holomorphic on ''D'', thus an extension of ''f''.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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