The spin group ,
for
, is the connected double
cover of the special orthogonal group
. It can be constructed inside the
group of units of the Clifford algebra of
as products of an even number of unit vectors. Conjugation on vectors
gives an exact sequence
The spinor representations of arise from its action through the Clifford
algebra and do not descend to
. However, failure to descend does not characterize the
spinor representations (Woit 2017, Chs. 7 and 31).