PlanetPhysics/Clifford Algebra

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A Noncommutative Quantum Observable Algebra is a Clifford Algebra

Let us briefly define the notion of a Clifford algebra . Thus, let us consider first a pair (V,Q), where V denotes a real [[../NormInducedByInnerProduct/|vector space]] and Q is a quadratic form on V~. Then, the Clifford algebra associated to V , is denoted here as Cl(V)=Cl(V,Q), is the algebra over Failed to parse (unknown function "\bR"): {\displaystyle \bR} generated by V , where for all v,wV, the [[../Bijective/|relations]]: vw+wv=2Q(v,w), are satisfied; in particular, v2=2Q(v,v)~.

If W is an algebra and Failed to parse (unknown function "\lra"): {\displaystyle c : V \lra W} is a linear map satisfying c(w)c(v)+c(v)c(w)=2Q(v,w), then there exists a unique algebra [[../TrivialGroupoid/|homomorphism]] Failed to parse (unknown function "\lra"): {\displaystyle \phi : \mbox{Cl}(V) \lra W} such that the [[../Commutativity/|diagram]]

Failed to parse (unknown function "\xymatrix"): {\displaystyle \xymatrix{&&\hspace*{-1mm}\mbox{Cl}(V)\ar[ddrr]^{\phi}&&\\&&&&\\ V \ar[uurr]^{\mbox{Cl}} \ar[rrrr]_&&&& W}}

[[../Commutator/|commutes]]. (It is in this sense that Cl(V) is considered to be `universal').

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