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Encyclopedia > Removable singularity

In complex analysis, a removable singularity of a function is a point at which the function is not defined (a singularity) but at which the function can be defined without creating any problems. "Problems" would be discontinuity or non-differentiability.


For instance, the function f(z) = sin(z)/z for z ≠ 0 has a removable singularity at z = 0: we can define f(0) = 1 and the resulting function will be continuous and even differentiable (a consequence of L'Hopital's rule).


Formally, if U is an open subset of the complex plane C, a is an element of U and f : U - {a} → C is a holomorphic function, then z is called a removable singularity for f if there exists a holomorphic function g : UC which coincides with f on U - {a}. Such a holomorphic function g exists if and only if the limit limza f(z) exists; this limit is then equal to g(a).


Riemann's theorem on removable singularities states that the singularity a is removable if and only if there exists a neighborhood of a on which f is bounded.


The removable singularities are precisely the poles of order 0.


See also: analytic capacity


  Results from FactBites:
 
PlanetMath: potential theory (1101 words)
To the extent that it is possible to draw a distinction between these two fields, the difference is more one of emphasis than subject matter and rests on the following distinction -- potential theory focuses on the properties of the functions as opposed to the properties of the equation.
In this connection, a surprising fact is that many results and concepts originally discovered in complex analysis (such as Schwartz's theorem, Morera's theorem, the Casorati-Weierstrass theorem, Laurent series, and the classification of singularities as removable, poles and essential) generalize to results on harmonic functions in any dimension.
As alluded to in the last section, one can classify the isolated singularities of harmonic functions as removable singularities, poles, and essential singularities.
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