Statement

On the positive-definite Hermitian-matrix model of , the formula

HAHA,ASL(2,C),H\longmapsto AHA^\dagger,\qquad A\in SL(2,\mathbb C),

is isometric and has kernel {±I}\{\pm I\}. It induces an isomorphism of real Lie groups

PSL(2,C)R    Isom+(H3).PSL(2,\mathbb C)_{\mathbb R} \xrightarrow{\;\sim\;} \operatorname{Isom}^+(\mathbb H^3).
Relation to the Lorentz model

Under the determinant-one hyperboloid model, this is the restriction of the to the sheet q(v)=1, t>0q(v)=-1,\ t>0. Consequently,

Isom+(H3)SO+(1,3)PSL(2,C)R.\operatorname{Isom}^+(\mathbb H^3) \cong SO^+(1,3) \cong PSL(2,\mathbb C)_{\mathbb R}.

These isomorphisms are in the category of real Lie groups.

Boundary action and quotients

The action extends continuously to H3CP1\partial_\infty\mathbb H^3\cong\mathbb{CP}^1, where it is the . Thus a Γ<PSL(2,C)\Gamma<PSL(2,\mathbb C) acts simultaneously on H3\mathbb H^3 and its sphere at infinity. The quotient Γ\H3\Gamma\backslash\mathbb H^3 is a hyperbolic orbifold, and is a manifold when Γ\Gamma acts freely. Arithmetic choices of Γ\Gamma connect this geometry with automorphic forms and representation theory.

References
  1. John G. Ratcliffe, Foundations of Hyperbolic Manifolds, 3rd ed., Springer, 2019, §§3.2–3.3 and 4.5. Publisher record.
  2. Alan F. Beardon, The Geometry of Discrete Groups, Springer, 1983, Chapters 4 and 7. Publisher record.