I'm trying to prove that $SL(2,\mathbb{C})$ is the universal covering group for the proper orthochronous Lorentz group $SO(1,3)^{\uparrow}$. The standard way goes as follows.
(1) Exhibit a real vector space isomorphism between Minkowski space and the space of $2\times 2$ Hermitian matrices, $H$.
(2) Let $SL(2,\mathbb{C})$ act on $H$ by $X\mapsto AXA^{\dagger}$ and prove this induces a surjective, 2:1 homomorphism from $SL(2,\mathbb{C})$ to $SO(1,3)^{\uparrow}$.
I'm wondering whether there is a better way however. To prove that $SU(2)$ is the universal covering group of $SO(3)$ it suffices to go to the Lie algebra and demonstrate that the adjoint representation is an isomorphism of Lie algebras. Can I do something analogous here?
Here's what I've tried. The Lie algebra of $SO(1,3)$ is $su(2)\oplus su(2)$ which naturally acts on a 4-dimensional complex vector space. The Lie algebra of $SL(2,\mathbb{C})$ is the space of traceless complex matrices, of dimension 6. I can't now see how to proceed.
Maybe this approach doesn't work at all now. Is it just a special property of $SU(2)$ and $SO(3)$ that happens because $SU(2)$ happens to have dimension 3, exactly the right number for an $SO(3)$ action?
Many thanks in advance!