Definition

Let VV be a over a commutative kk in which 22 is invertible, and let q:Vkq:V\to k be a quadratic form. The Clifford algebra Cl(V,q)\operatorname{Cl}(V,q) is the unital associative algebra

Cl(V,q)=T(V)/vv+q(v)1:vV.\operatorname{Cl}(V,q) =T(V)\big/\langle v\otimes v+q(v)1:v\in V\rangle .

Thus the image of every vVv\in V satisfies v2=q(v)1v^2=-q(v)1. If q(v)=g(v,v)q(v)=g(v,v) comes from an , polarization gives

vw+wv=2g(v,w)1.vw+wv=-2g(v,w)1.

This sign is the common Riemannian-geometry convention; many algebra texts instead impose v2=q(v)1v^2=q(v)1.

Universal property

The quotient is characterized without choosing a basis. If AA is any unital associative kk-algebra and f:VAf:V\to A is linear with

f(v)2=q(v)1A,f(v)^2=-q(v)1_A,

then there is a unique unital

f~:Cl(V,q)A\widetilde f:\operatorname{Cl}(V,q)\to A

whose restriction to VV is ff. This property makes natural under isometries of quadratic spaces.

Grading and dimension

The tensor-degree parity descends to a Z/2\mathbb Z/2-grading

Cl(V,q)=Cl0(V,q)Cl1(V,q).\operatorname{Cl}(V,q) =\operatorname{Cl}^0(V,q)\oplus\operatorname{Cl}^1(V,q).

Vectors lie in the odd part, while products of an even number of vectors lie in the even part. If VV is free of finite rank nn, then the usual ordered monomials in a basis show that Cl(V,q)\operatorname{Cl}(V,q) has rank 2n2^n as a kk-module, without requiring qq to be nondegenerate.

Real and complex forms

For a real quadratic space one obtains a real Clifford algebra, whose isomorphism type depends on the signature and displays mod-88 periodicity. Complexification gives

ClC(V,q)=ClR(V,q)RC.\operatorname{Cl}_{\mathbb C}(V,q) =\operatorname{Cl}_{\mathbb R}(V,q)\otimes_{\mathbb R}\mathbb C.

Over C\mathbb C, the signature no longer affects the isomorphism type, although parity of dimV\dim V still matters.

Sign warning

Two standard conventions coexist:

v2=q(v)1orv2=q(v)1.v^2=-q(v)1 \qquad\text{or}\qquad v^2=q(v)1.

They interchange some signature labels and change the displayed Clifford relation. A formula for spinors or is therefore meaningful only after its sign convention has been fixed.

References
  1. H. Blaine Lawson Jr. and Marie-Louise Michelsohn, Spin Geometry, Princeton University Press, 1989. DOI record. Relevant: Chapter I, Clifford algebras and modules.
  2. Nicole Berline, Ezra Getzler, and Michèle Vergne, Heat Kernels and Dirac Operators, Springer, 1992. DOI record. Relevant: Chapter 3, Clifford algebras.