Question about Green, Schwarz, Witten Appendix 4.A on N=1SYM

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In summary, the conversation discussed the use of spinors in different dimensions, with a focus on Majorana and Majorana-Weyl spinors. The use of these spinors is determined by the representation theory of Clifford Algebras and their periodicity. Some recommended references for further understanding are mentioned, including the appendix of Polchinski's book and several articles and demonstrations.
  • #1
petergreat
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It's really just a dumb question about spinors. The book says that for N=1 SYM, in 3 or 4D we use Majorana spinors. In 6D we use Weyl spinors. And in 10D we use Majorana-Weyl spinors, so that the number of fermionic states matches D-2.

My questions is, in 4D, Weyl spinors (chiral spinors) also have only 2 degrees of freedom. Why must we use Majorana spinors instead?

In which dimensions do Majorana spinors exist? And which dimensions allow Majorana-Weyl spinors? What are the gamma matrices in these representations? What's the best reference for these issues?

Thanks in advance.
 
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  • #2
For a short review, I would suggest the appendix of the 2nd volume of Polchinski's book.
 
  • #3
Sorry for the late post.

It's got to do with the representation theory of Clifford Algebras and its modulo 8 (Bott) periodicity.
Some references are:
Clifford Algebras in Physics: http://arxiv.org/abs/hep-th/0506011
The Pin Groups in Physics: C, P, and T: http://arxiv.org/abs/math-ph/0012006
http://demonstrations.wolfram.com/TrigramsAndRealCliffordAlgebras/

The first one is a nice clear short discussion that should answer all of the questions you posed in your post. The second reference has some really interesting material by some of the people most knowledgeable about this stuff. The final reference is just some pretty pictures that I made.
 

Related to Question about Green, Schwarz, Witten Appendix 4.A on N=1SYM

1. What is the purpose of Appendix 4.A on N=1SYM in the Green, Schwarz, Witten theory?

The purpose of Appendix 4.A is to provide a detailed explanation and derivation of the N=1 super Yang-Mills (SYM) theory. It serves as a reference for understanding the mathematical and theoretical foundations of the theory.

2. What is N=1SYM theory and why is it important?

N=1SYM theory is a supersymmetric quantum field theory that describes the interactions between particles at the subatomic level. It is important because it helps us understand the behavior of fundamental particles and their interactions, and it is a key component of the broader study of string theory.

3. What are some key concepts discussed in Appendix 4.A?

Some key concepts discussed in Appendix 4.A include the supersymmetry algebra, superfields, and the superfield action. These concepts are essential for understanding the N=1SYM theory and its applications.

4. How does Appendix 4.A contribute to our understanding of string theory?

Appendix 4.A provides a mathematical framework for understanding N=1SYM theory, which is a crucial component of string theory. It helps us understand the behavior of strings and their interactions in a more precise and comprehensive manner.

5. Are there any practical applications of the N=1SYM theory described in Appendix 4.A?

Yes, the N=1SYM theory has practical applications in theoretical physics, particularly in the study of quantum field theory and string theory. It also has potential applications in fields such as cosmology and condensed matter physics.

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