The Poincare disc model is
Its geodesics through the origin are the Euclidean diameters. To see directly that the radial segment from to minimizes length, write an arbitrary joining curve as . Its hyperbolic length satisfies
The radial segment has constant and monotone , so equality holds. Hence
and every radial diameter is length minimizing. Rotational symmetry and uniqueness for the geodesic equation show that these are all geodesics through .
Given any geodesic and a point on it, a disc-preserving map
takes to the origin. By part (a), is a hyperbolic isometry and commutes with . The transformed geodesic is a diameter, hence a generalized circle invariant under . Its inverse image is therefore also a Generalized circle under a Möbius transformation invariant under . Thus every hyperbolic geodesic is the part in of a Euclidean line or circle preserved by reflection in the unit circle; equivalently, it is a diameter or a circle orthogonal to the unit circle. This is the Geodesics of the Poincare disc description.
A Möbius transformation is generated by translations , nonzero scalings , and inversion . Translations and scalings plainly take circles and lines to circles and lines. More uniformly, every circle or line has an equation
where ; the case is a line. Under inversion, put and multiply by to obtain
which is again such an equation. The generators, and hence every Möbius transformation, therefore preserve Generalized circle under a Möbius transformation.
Now let
If , its finite pole lies on some Euclidean circle, and that circle maps to a line because its image contains infinity. Thus takes every circle to a circle exactly when , so the subgroup in question is the Affine subgroup of the Möbius group, consisting of with .
It is not normal. If and with , then is affine but
has a finite pole and is not affine. Hence conjugation by does not preserve the subgroup.