Definition (via the Clifford algebra)
Let V=Rn with its standard inner product ⟨⋅,⋅⟩, and let Cl(V) be the real Clifford algebra generated by V subject to the relations
v⋅v=−⟨v,v⟩1(v∈V).
The spin group Spin(n) is the subgroup of the even Clifford algebra Cl0(V) generated by products of an even number of unit vectors:
Spin(n)=⟨v1v2⋯v2k∣vi∈V, ⟨vi,vi⟩=1⟩⊂Cl0(V)×.
Covering map to SO(n)
There is a canonical group homomorphism
ρ:Spin(n)→SO(n)
defined by the conjugation action on V⊂Cl(V):
ρ(s)(v)=svs−1.
One checks that ρ(s) preserves ⟨⋅,⋅⟩ and has determinant 1, hence lands in the special orthogonal group SO(n). Moreover,
ker(ρ)={±1},
so ρ is a 2-fold covering map. For n≥3, Spin(n) is connected and simply connected, and ρ identifies it as the universal covering group of SO(n).
Lie algebra and context
The differential dρe is an isomorphism of Lie algebras, so the Lie algebra of Spin(n) is canonically identified with the orthogonal Lie algebra mathfrakso(n). This makes Spin(n) fundamental in topology and representation theory: “spin representations” are representations of Spin(n) that do not descend to SO(n), reflecting the nontriviality of the covering.