Identify the projective line with one-dimensional subspaces of : use for finite , and . This convention turns the matrix action into the stipulated Möbius transformation.
Since and are distinct projective points, are a basis. Write . Both and are nonzero, because is different from . The matrix with columns and is invertible and sends the lines of to those of , respectively. This constructs the requested map without separate exceptional formulas at infinity.
A matrix fixing and is diagonal, say with . To fix it must also satisfy , so the stabilizer subgroup of is precisely . Any two solutions differ on the right by one of these matrices. Thus
Equivalently, after dividing out scalar matrices the projective general linear group action on the projective line is sharply three-transitive on a projective line.
The Möbius transformations are bijections, so they preserve which coordinates of a triple are equal. Conversely, part (i) implies transitivity within each equality pattern. For a pattern with fewer than three distinct entries, extend the chosen distinct points to a triple before applying part (i); this works also for , when the projective line has exactly three points. There are therefore five orbits of a group action.
We first count . Its first column can be any nonzero vector, giving choices. The second must be outside the first column's one-dimensional span, giving choices. Hence
For the all-equal pattern take . Its stabilizer subgroup consists of upper triangular matrices
of order . Its group orbit has order .
The three exactly-two-equal patterns have representatives , and . Each stabilizer subgroup fixes and individually, so it is the diagonal subgroup of order . Each group orbit has order ; their repeated-coordinate positions keep these three orbits distinct.
For the all-distinct pattern use . Its stabilizer subgroup is the scalar subgroup of order , and the group orbit has order . Stabilizers of arbitrary triples are conjugates of the displayed representative stabilizers. In summary the equality-pattern orbits of projective triples have
The sizes add to , and each orbit size times its stabilizer order is , as in the orbit-stabilizer theorem.

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