Let n≥2n\ge 2, let V=RnV=\mathbb R^n with its standard inner product ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle, and let Cl(V)\mathrm{Cl}(V) be the real Clifford algebra generated by VV subject to the relations

v⋅v=−⟨v,v⟩ 1(v∈V).v\cdot v=-\langle v,v\rangle\,1 \quad (v\in V).

The spin group Spin(n)\mathrm{Spin}(n) is the subgroup of the even Clifford algebra Cl0(V)\mathrm{Cl}^0(V) generated by products of an even number of unit vectors:

Spin(n)=⟨v1v2⋯v2k∣vi∈V, ⟨vi,vi⟩=1⟩⊂Cl0(V)×.\mathrm{Spin}(n)=\langle v_1v_2\cdots v_{2k}\mid v_i\in V,\ \langle v_i,v_i\rangle=1\rangle \subset \mathrm{Cl}^0(V)^\times.
Covering map to SO(n)SO(n)

There is a canonical group homomorphism

ρ:Spin(n)→SO(n)\rho:\mathrm{Spin}(n)\to SO(n)

defined by the conjugation action on V⊂Cl(V)V\subset \mathrm{Cl}(V):

ρ(s)(v)=s v s−1.\rho(s)(v)=s\,v\,s^{-1}.

One checks that ρ(s)\rho(s) preserves ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle and has determinant 11, hence lands in the . Moreover,

ker⁡(ρ)={±1},\ker(\rho)=\{\pm 1\},

so ρ\rho is a 22-fold covering map. For n≥3n\ge 3, Spin(n)\mathrm{Spin}(n) is connected and simply connected, and ρ\rho identifies it as the of SO(n)SO(n).

Lie algebra and context

The differential dρed\rho_e is an isomorphism of Lie algebras, so the Lie algebra of Spin(n)\mathrm{Spin}(n) is canonically identified with the so(n)\mathfrak{so}(n). This makes Spin(n)\mathrm{Spin}(n) fundamental in topology and representation theory: “spin representations” are representations of Spin(n)\mathrm{Spin}(n) that do not descend to SO(n)SO(n), reflecting the nontriviality of the covering.

Positive-definite scope

This knowl uses a positive-definite inner product, which has signature (0,n)(0,n) in this collection's negative-first ordering, and the Clifford convention v2=−⟨v,v⟩v^2=-\langle v,v\rangle. For a quadratic form of mixed signature, the related groups Pin⁡(p,q)\operatorname{Pin}(p,q), Spin⁡(p,q)\operatorname{Spin}(p,q), and their identity components require additional component bookkeeping; see . In the Lorentzian case,

Spin⁡+(1,3)≅SL(2,C)R.\operatorname{Spin}^+(1,3)\cong SL(2,\mathbb C)_{\mathbb R}.

This link does not redefine the compact group Spin⁡(n)\operatorname{Spin}(n) treated above.

References
  1. H. Blaine Lawson and Marie-Louise Michelsohn, Spin Geometry, Princeton University Press, 1989, Chapter I, §§2–5. Publisher record.
  2. Thomas Friedrich, Dirac Operators in Riemannian Geometry, AMS, 2000, §1.3. Publisher record.