This is a follow up to this question. Since global phases are unphysical in quantum mechanics we often consider projective representations, where the matrices are defined only modulo a global $ e^{i\theta} $, instead of true linear representations. It turns out that the projective representations of $ G $ correspond exactly to the linear representations of the universal cover which is a central extension of the original group. For example $ SO_3 $ has universal cover $ SU_2 $ and projective representations of $ SO_3 $ correspond to half-integer spin in quantum mechanics.
- This story for semisimple Lie groups has an analogue in the theory of perfect finite groups. For a perfect group $ G $ there is a universal central extension, sometimes called the universal cover, with the property that the projective representations of $ G $ are in exact correspondence with the linear representations of the universal cover.
- In the theory of semisimple Lie groups, a group which is its own universal cover is called simply connected. This is equivalent to the fundamental group of $ G $ being trivial. For a semisimple Lie group the fundamental group is always a finite Abelian group.
- In the theory of perfect groups a group which is its own universal cover is called superperfect, this is equivalent to the Schur multiplier being trivial. For a perfect finite group the Schur multiplier is always a finite Abelian group.
The Clifford group $ \overline{Cl}_n$ (the automorphism group of the Pauli group $ P_n $ ) is a perfect group which is important in quantum computing. I want to know if $ \overline{Cl}_n$ is superperfect or if the there exists some nontrivial perfect central extensions (i.e. the Schur multiplier is nontrivial). If the Schur multiplier is nontrivial I would certainly be curious which finite Abelian group it is.
 
    