An isolated singularity at means that is holomorphic in some punctured disk , while itself is an excluded point or a point where the given function is not holomorphic. There are no other singularities arbitrarily close to . By Laurent's theorem, the function has a unique Laurent series on that punctured disk:The negative-power terms form its principal part of a Laurent series.
A removable singularity is an isolated singularity for which the function on the punctured disk extends to a holomorphic function on the full disk, by assigning or correcting its value at . In Laurent series terms,The remaining power series defines the extension with value at . Conversely, a holomorphic extension has a Taylor series there, so uniqueness of the Laurent series forces all negative coefficients to vanish.
A pole of order at has finitely many negative powers in its Laurent series, the lowest being exactly :Equivalently,Thus has a holomorphic extension with nonzero value at , whereas multiplying by any smaller power does not remove the singularity.
A zero of order at means that is holomorphic near andEquivalently its Taylor series starts with the nonzero coefficient of , soUnlike a pole, a zero is a regular point of the function itself; its reciprocal has a pole of the corresponding order.
By the finite-order zero factorizations,with holomorphic near . Shrinking the disk if necessary, continuity ensures never vanishes there, so is holomorphic and nonzero at . ConsequentlyIf , the exponent is , with a holomorphic nonvanishing factor. Hence
With the same factors, if , thenhas no negative power and extends holomorphically across . Thus its apparent singularity is a removable singularity, with extension valueFor the extended quotient has a zero of order ; for the extension is nonzero.
The complex sine has simple zeros exactly at , , because and . Hence the denominator has a zero of order three at each of these points and nowhere else.
At , the numerator has order two, so the quotient has a simple pole. Indeed its leading term is . At , the numerator has order one, so there is a pole of order two. At , the numerator has order three, cancelling the denominator's order-three zero, so the singularity is removable. Its extension value isAt every remaining , the numerator is nonzero, giving a pole of order three. Thus the complete finite-plane classification isAway from this discrete set the denominator is nonzero, so the quotient is holomorphic.
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