What is the Center of a Clifford Algebra of Order 2^n?

In summary, the center of a Clifford algebra of order 2^n is of order 1 if n is even, and 2 if n is odd. This is because for n even, only the unit element \gamma_0 commutes with all the other bases, while for n odd, both \gamma_0 and \gamma_{\{1,2,...,n\}} commute with all the other bases. It can also be shown that the center is spanned by the bases that commute with all the other bases, as no linear combinations of non-commuting bases can commute with all bases.
  • #1
sunjin09
312
0

Homework Statement



Show that the center of a Clifford algebra of order 2^n is of order 1 if n is even, and 2 if n is odd

Homework Equations


the center of an algebra is the subalgebra that commutes with all elements
Clifford algebra of 2^n is defined as being spanned by the bases
[itex]\gamma_0,\gamma_1,...\gamma_n[/itex]
where [itex]\gamma_0[/itex] is the unit element, as well as
[itex]\gamma_{\{n_k\}}=\Pi_{n_k}\gamma_{n_k}[/itex]
where [itex]1\le n_k\le n[/itex], and the mutiplication rule is
[itex]\gamma_u\gamma_v+\gamma_v\gamma_u=2\delta_{u,v} \gamma_0[/itex]
where [itex]\delta[/itex] is the Kronecker Delta symbol

The Attempt at a Solution



I was able to show that for n even, only [itex]\gamma_0[/itex] commutes with all the other bases
and for n odd, only [itex]\gamma_0[/itex] and [itex]\gamma_{\{1,2,...,n\}}[/itex] commutes with all the other bases, but
how can I know that the center is spanned by the bases that commutes with
all the other bases?

In other words, how do I know that no linear combinations of
non-commuting bases commutes to all bases?
 
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  • #2
I finally figured it out. Two things need to be realized:
1.All the basis elements are invertible
2.Any pair of the basis elements either commute with each other or anti-commute with each other;
These may be verified fairly easily from the definition.

Now if x is in the center, x must commute with all the basis elements. For any basis element γ, x may be
written as x=x1+x2, where x1γ=γx1 and x2γ=-γx2; since xγ=γx, we have x2γ=0; since γ is invertible, x2=0;
since x2 which depends on γ equals 0 for all γ, x must contain only components that commutes with all basis,
i.e., γ0 and possibly γ{1,2,...,n}, qed.

fairly straightforward, it feels good to know the answer. Anyone has a simpler proof?
 

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