Every nonidentity biholomorphism in the finite group has only finitely many fixed points, by the identity theorem on a Riemann surface and compactness. Because the group action is a faithful group action, the union of these finite sets does not exhaust . A point outside this union has trivial stabilizer subgroup, so its group orbit has points by the orbit-stabilizer theorem. The generic fiber of a function of the projection is such an group orbit, giving
More precisely, put and . Differentiation at gives a group homomorphism . It is injective: if a nonidentity finite-order germ had the form with and , then its th iterate would begin , so no positive iterate could be the identity. A germ equal to the identity gives the identity on by the identity theorem on a Riemann surface. Thus is a cyclic group, with derivative image the th roots of unity.
For completeness, an explicit local coordinate linearizing is
It has , and reindexing the sum gives . Therefore a coordinate on the local quotient space is . Other translates of a sufficiently small neighbourhood of are disjoint unless their translating element lies in , so this local quotient space is also a chart for . The local cyclic quotient of a Riemann surface consequently gives
Choose a local coordinate with . Differentiation at gives a homomorphism
It is injective. Indeed, a nonidentity Möbius transformation fixing and having derivative one there is parabolic, hence conjugate to a nonzero translation and of infinite order; no such element can belong to the finite group . Every finite subgroup of is a cyclic group of roots of unity, so is cyclic. Write .
The averaged coordinate
has derivative one at , so it is a coordinate on a smaller neighbourhood. For , reindexing by gives
After shrinking to an -invariant disc , the group therefore acts as all rotations , where is a primitive th root of unity. The invariant coordinate
identifies with a disc and gives it a Riemann-surface chart. In these coordinates the quotient map is exactly
This is the local cyclic quotient of a Riemann surface.