Homogenizing the affine equation gives the projective closure
This is the Klein quartic. It is smooth: if all three projective partial derivatives vanished, then
Multiplying them gives . If one coordinate is zero, the displayed equations force all three to vanish, which is impossible in projective space. Thus is a smooth compactification of . The smooth compactification compatible with the extended coordinate functions is its normalization, and since is already smooth it is biholomorphic to .
For a direct genus computation, consider the extended coordinate map . A generic leaves the cubic equation
so . In the affine part, ramification occurs where . Solving gives and the seven points
At the origin, , so the ramification index of a holomorphic map is three and the contribution is two. At each of the other seven points, , , and , so the ramification index is two and each contributes one.
There are two points at infinity. Near , in coordinates , , the equation is
and , so is unramified. Near , in coordinates , , the equation is
Thus and , so has ramification index two and contributes one. The total ramification is therefore
The Riemann-Hurwitz formula for the degree-three map to the sphere gives
and hence
This also agrees with the genus of a smooth plane curve of degree four.
Let be a nonconstant holomorphic map of degree between compact connected Riemann surfaces. At , let be the ramification index of a holomorphic map. Choose a triangulation of containing every branch value among its vertices, and lift it to .
If the target triangulation has vertices, edges, and triangles, then the lifted triangulation has edges and triangles, because no branch value lies in an edge or face interior. For a target vertex , local degree counting gives
Consequently the number of vertices above is
Writing , the Euler characteristic is therefore
Since a compact orientable surface of genus has Euler characteristic , this Triangulation proof of the Riemann-Hurwitz formula gives
or equivalently
Now extend a cubic polynomial to a degree-three holomorphic map
of the Riemann sphere. Both genera are zero, so Riemann--Hurwitz gives
The point at infinity is totally ramified with , contributing two. Thus the finite points contribute exactly two. There are consequently two cases.
If there is one finite ramification point , it has index three. Choose an affine source map sending zero to . Then
for some , and integration gives
An affine target map subtracts and rescales by , yielding .
Otherwise there are two distinct finite ramification points, each of index two. Choose an affine source map sending and to them. The derivative of is then a nonzero multiple of :
Hence
The affine target map gives
Therefore the affine normal forms of a complex cubic polynomial are precisely
In local coordinates centred at and , a nonconstant rational map has the form
The point is a ramification point of a holomorphic map when its ramification index of a holomorphic map satisfies . A branch value of a holomorphic map, also called a branch point in the target, is a value of some ramification point.
Let be the finite set of branch values and put . For every , all points of have local degree one, so the holomorphic inverse function theorem supplies disjoint neighbourhoods on which is biholomorphic. Compactness of the fibre lets their target neighbourhoods be intersected to one evenly covered neighbourhood of . Hence
is an unramified covering map. Here the displayed restriction requires ; if “ramification point” is reserved only for points with , then the source deletion must be written .
The Monodromy theorem says that analytic continuations along endpoint-fixed homotopic paths have the same terminal germ. Equivalently here, the path lifting theorem lifts a loop based at from each point of ; taking the endpoint of each lift permutes that fibre. The permutation depends only on , giving the monodromy group of a covering.
For the stated function, make the Möbius change of coordinate
Then
The critical points are , with branch values
A loop around interchanges the two roots born from , so its branch cycle is a transposition. A loop around simultaneously interchanges the two pairs that collide there, so its branch cycle is a product of two disjoint transpositions. With a suitable labelling these are
They generate a transitive group of order eight; their product is a four-cycle. Therefore the full monodromy group is
the dihedral group in its action on the four vertices of a square.