π-monoid
Clifford algebra
Let (π,π) be a quadratic space over π.
The Clifford algebra Clβ‘(π,π) is the freΓ«st π-monoid generated by π subject to the condition to #m/def/ralg/geo
π£2=π(π£)1
as formalized by the universal property.
Away from 2, this is equivalent to the freΓ«st unital associative algebra such that the anticommutator extends the polar form
{π£,π€}=π£π€+π€π£=ππ(π£,π€)1
This motivates yet another perspective: Clβ‘(π,π) is the freΓ«st unital associatve algebra whose associated Jordan algebra π΄+ has a product extending ππ,
i.e. π΄+1/2 has a product extending ( β) β
( β).
In a sense the Clifford algebra generalizes, or rather quantizes the Exterior algebra.
It is sometimes called the orthogonal Clifford algebra, as opposed to the related Weyl algebra which is sometimes called the symplectic Clifford algebra.
Universal property
Let (π,π) be a quadratic space over π.
The associated Clifford algebra is a pair consisting of a π-monoid Clβ‘(π,π) and a linear map π :π βClβ‘(π,π) with the identity π(π£)2 =π(π£)1
such that given any unital associative algebra π΄, a linear map π :π βπ΄ satisfying π(π£)2 =π(π£)1 factorizes uniquely through π
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such that Β―π :Clβ‘(π,π) βπ΄ is a unital algebra homomorphism.
This admits a unique extension to a functor Cl :π°π΅πΎπΌππ βπ΄π ππ π
ππ such that π :1 βCl :π°π΅πΎπΌππ βπ΅πΎπΌππ becomes a natural transformation.
Construction
The Clifford algebra may be constructed as a quotient algebra of the tensor algebra
Clβ‘(π,π)=πβπβ¨π£βπ£βπ(π£):π£βπβ©β΄πβπ
where the divisor is the algebra ideal generated by tensors of the form π£ βπ£ βπ(π£)1.
Proof of the universal property
Relation to the exterior algebra
The exterior algebra is the associated graded algebra of the Clifford algebra, whence there is a natural linear isomorphism between them.
With this identification, we have
πβπ=1π£π=1π!βπβππsgnβ‘(π)πβπ=1π£π
We carry over all the terminology, referring to π-vectors, &c.
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