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Every isolated singularity is removable, a pole, or essential
Statement
Let be holomorphic on a punctured disc . Then exactly one of the following holds:
- is a removable singularity of ;
- is a pole of ;
- is an essential singularity of .
Equivalently, if
then the three cases are: no negative coefficients, finitely many negative coefficients but not all zero, or infinitely many negative coefficients.
Facts & Assumptions
Given: A function holomorphic on and its Laurent expansion there.
A removable singularity is exactly the case of zero principal part (Characterizations of removable singularities).
A pole is exactly the case of a finite nonzero principal part (Characterizations of poles).
An essential singularity is, by definition, an isolated singularity that is neither removable nor a pole (Isolated singularities: removable, poles, and essential singularities).
Every holomorphic function on a punctured disc has a Laurent expansion there (Laurent expansion on an annulus).
Proof
By [L4], the Laurent expansion exists, and its set of negative coefficients is either empty, finite nonempty, or infinite.
If there are no negative coefficients, the principal part is zero, so [L1] makes the singularity removable.
If there are finitely many negative coefficients and at least one is nonzero, the principal part is finite and nonzero, so [L2] makes the singularity a pole.
If there are infinitely many negative coefficients, the singularity is neither removable nor a pole by steps 2.1 and 2.2, so [L3] makes it essential.
The three coefficient cases are mutually exclusive and exhaustive, and steps 2.1 through 3.1 identify them with the three singularity types.
Depends on
Used by
- e^1/z has an essential singularity at 0 and omits the value 0 Counterexample
- sin(1/z) has an essential singularity at 0 Counterexample
- Casorati-Weierstrass theorem Theorem
Dependency tree · two levels
20 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- Jean-Baptiste Campesato, MAT334 course page and notes index (standard reference, not scraped)
- David Greenfield, Rutgers Math 403 diary (standard reference, not scraped)