Isomorphism between Clifford algebras CL(4,2) and CL(2,4)

  • Context: Graduate 
  • Thread starter Thread starter mnb96
  • Start date Start date
  • Tags Tags
    Isomorphism
Click For Summary
SUMMARY

The discussion centers on the isomorphism between the Clifford algebras \(\mathcal{C}\ell_{4,2}(\mathbb{R})\) and \(\mathcal{C}\ell_{2,4}(\mathbb{R})\). The author references a book that claims these algebras are isomorphic based on their signatures. Participants clarify that the anti-commutator notation \(\{A,B\}\) is used, and the metric tensor \(\eta\) is involved in the algebra's structure. The conclusion drawn is that while the isomorphism holds over \(\mathbb{C}\), it does not necessarily apply over \(\mathbb{R}\), emphasizing the physical equivalence of the algebras despite their different signatures.

PREREQUISITES
  • Understanding of Clifford algebras, specifically \(\mathcal{C}\ell_{p,q}(\mathbb{R})\)
  • Familiarity with anti-commutator notation in algebra
  • Knowledge of metric tensors and their role in defining algebraic structures
  • Basic concepts of isomorphism in algebraic systems
NEXT STEPS
  • Study the properties of Clifford algebras, focusing on \(\mathcal{C}\ell_{p,q}(\mathbb{R})\)
  • Learn about the implications of isomorphism in algebra over different fields, particularly \(\mathbb{R}\) and \(\mathbb{C}\)
  • Investigate the relationship between the special orthogonal groups \(SO(p,q)\) and \(SO(q,p)\)
  • Explore applications of Clifford algebras in physics, especially in the context of spacetime and conformal algebras
USEFUL FOR

Mathematicians, physicists, and students of algebra interested in the properties and applications of Clifford algebras, particularly in theoretical physics and geometry.

mnb96
Messages
711
Reaction score
5
Hi,

I was reading a paragraph of a book (you can find it here) where the author seems to suggest that the Clifford algebras \mathcal{C}\ell_{2,4}(\mathbb{R}) and \mathcal{C}\ell_{4,2}(\mathbb{R}) are isomorphic. In particular, at the third line after Equation (10.190), when he talks about the algebra with signature (4,2), the authors says:

"The signature shows that this space is isomorphic to the conformal algebra of spacetime"

where by "conformal algebra of spacetime" he means the algebra with signature (2,4).

How did he manage to deduce just from the signatures of these two algebras that they are indeed isomorphic?
I am not convinced of this statement, and I am wondering if there is a quick way to prove it (that I am missing).

Thanks!
 
Physics news on Phys.org
The Clifford algebra is generated by matrices ##\Gamma_\mu## satisfying

$$\{ \Gamma_\mu, \Gamma_\nu \} = 2 \eta_{\mu\nu}$$
To flip ##\eta_{\mu\nu} \to - \eta_{\mu\nu}##, just send ##\Gamma_\mu \to i \Gamma_\mu##.
 
Hi Ben,

thanks a lot for answering, though I must confess that I didn't understand anything of what you wrote.
In particular, I don't know what \Gamma and \eta stand for, and I have never seen the notation \{A,B\}. Could you please clarify this?
Thanks.
 
Sorry, but I don't think my original question received an answer.

Assuming that in Ben's first equation the curly braces denote the anti-commutator, and assuming that η in the right-term denotes the metric tensor (btw the identity matrix next to η is missing), then I don't see how the trick of sending ##\Gamma_\mu \to i \Gamma_\mu## could automatically prove that we have created a Clifford algebra isomorphism.

It seems to me that we could apply, for instance, the same reasoning to the generating elements of ##\mathcal{C}\ell_{2,0}(\mathbb{R})## and prove that: ##\mathcal{C}\ell_{2,0}(\mathbb{R})\simeq \mathcal{C}\ell_{0,2}(\mathbb{R}) \simeq \mathbb{H}## which is clearly not true.

I hope someone can answer my original question.
 
Good points. Since the map I've written involves multiplication by ##i##, it only establishes the isomorphism of the algebras over ##\mathbb{C}##, not over ##\mathbb{R}##. But I think for any practical purpose, that is enough. I know it makes no physical difference whether you work in a Clifford algebra of signature (p,q) or of (q,p). It should be obvious that ##SO(p,q) \simeq SO(q,p)##, so either Clifford algebra can be used to construct 1/2-integer representations.
 

Similar threads

  • · Replies 14 ·
Replies
14
Views
5K
  • · Replies 4 ·
Replies
4
Views
1K
  • · Replies 5 ·
Replies
5
Views
1K
  • · Replies 21 ·
Replies
21
Views
1K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 11 ·
Replies
11
Views
5K
  • · Replies 2 ·
Replies
2
Views
5K
  • · Replies 1 ·
Replies
1
Views
654