We now have almost enough information to characterize the different types of Isolated Singularities. We list them here:

Removable Singularities
  1. (Analytic) Let f:UC be holomorphic on some open set UC. Suppose z0 is an isolated singularity of f, and let Br(z0){z0}U by definition. If the Laurant series of f 1;;vanishes, then z0 is a removable singularity
  2. (Geometric) Let f:UC be holomorphic on some open set UC. Suppose z0 is an isolated singularity of f, and accordingly let Br(z0){z0}U. Suppose there exists some Rr such that 1;;f is bounded on BR(z0){z0}, then by 11. Theorem 2.3.2 we have that z0 is a removable singularity.
Poles
  1. (Anayltic) Let f:UC be holomorphic on some open set UC. Suppose z0 is an isolated singularity of f, and let Br(z0){z0}U by definition. If the principal part of the Laurant Series 1;;is a polynomial (in 1x), then z0 is a pole of f.
  2. (Geometric) Let f:UC be holomorphic on some open set UC. Suppose z0 is an isolated singularity of f, and let Br(z0){z0}U by definition. If for all M>0, 1;;there exists some 0<ϵ<r such that |f(z)|>M for all zBϵ(z0){z0}, then z0 is a pole.
Essential Singularities
  1. (Analytic) Let f:UC be holomorphic on some open set UC. Suppose z0 is an isolated singularity of f, and let Br(z0){z0}U by definition. If the principal part of the Laurant Series is 1;;infinite, then z0 is an essential singularity.
  2. Let f:UC be holomorphic on some open set UC. Suppose z0 is an isolated singularity of f, and let Br(z0){z0}U by definition. Now suppose that there is some M>0 such 1;;that for any 0<ϵ<r there exists a zBϵ(z0){z0} such that |f(z)|M. Further suppose that |f| is unbounded in Bϵ(z0){z0}. Then z0 is an essential singularity of f. This has a more explicit characterization in the following theorem.
Remark

Notice that by the intermediate value theorem, we have that |f| hits every positive real number. What this means is that for every r>0, we can find a zU such that |f(z)|=r. Casorati and Weierstrauss go one step further and say essentially that f(Bϵ)δBr(0) is dense for every r.

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