The denominator factors as and neither factor cancels with the numerator. Thus there are simple poles at . At infinity the quotient tends to one and has a regular expansion in , so it has a removable singularity at infinity, with extended value one.
The numerator is nonzero at and , so the finite singularities are a pole of order three at and a pole of order two at . The numerator degree exceeds the denominator degree by three, with leading behaviour . Hence infinity is a pole of order three.
There are logarithmic branch points at and infinity. At zero, every local branch has , so division by gives a pole of order two at zero. Decay at infinity does not remove its branching: with , the function is , which changes branch when encircles zero.

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