Q&A on String Theory Course Indices/QFT

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The discussion revolves around various questions related to string theory, particularly focusing on indices and quantum field theory (QFT). Key points include the definition of spinor indices, which are associated with the representation of the Lorentz group, and the implications of transposing expressions involving Dirac spinors, which introduces minus signs due to anticommutation properties. Participants also explore the nature of the Polyakov action, confirming it describes a bosonic particle, and the derivation of left-moving wave solutions from specific equations of motion. Additionally, the handling of surface terms in integrals and the treatment of derivatives in the context of supersymmetry transformations are discussed, emphasizing the need for clarity in mathematical manipulations. Overall, the thread highlights intricate aspects of theoretical physics that require careful consideration of mathematical conventions and physical interpretations.
  • #31
fzero said:
The first expression he writes down is for flat space. The second one is correct for curved space because we're using the flat coordinates.

I still don't follow. I thought we were using the veirbein to put Latin indices in the curved case and basis indices for the flat case. Surely this would mean the 1st eqn would be for curved space and the second for flat.
 
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  • #32
latentcorpse said:
I still don't follow. I thought we were using the veirbein to put Latin indices in the curved case and basis indices for the flat case. Surely this would mean the 1st eqn would be for curved space and the second for flat.

There's two problems with trying to define spinors on a curved manifold. The first is that a general curved manifold is not invariant under Lorentz transformations, so you can't even define the transformation of a spinor in curved indices. You can define tensors because you have a GL(n) group acting on the tangent space, but GL(n) does not have spinor representations. So you must introduce local frames to define spinors.
 
  • #33
fzero said:
There's two problems with trying to define spinors on a curved manifold. The first is that a general curved manifold is not invariant under Lorentz transformations, so you can't even define the transformation of a spinor in curved indices. You can define tensors because you have a GL(n) group acting on the tangent space, but GL(n) does not have spinor representations. So you must introduce local frames to define spinors.

OK. This makes sense to me. Can you explain the choice of indices in those two equations though? Like, why does he chose latin for one and greek for the other?
 
  • #34
latentcorpse said:
OK. This makes sense to me. Can you explain the choice of indices in those two equations though? Like, why does he chose latin for one and greek for the other?

I expect that it's because you're using Latin indices for spacetime indices, whether spacetime is Minkowski or curved.
 
  • #35
fzero said:
I expect that it's because you're using Latin indices for spacetime indices, whether spacetime is Minkowski or curved.

so to summarise, the transformation in Minkowski space (the first one i wrote down) had latin indices because in Minkowski space we can define spinor transformations and this will hold in any basis so we can move to abstract indices.

However, in a curved spacetime we cannot define spinor transformations so we need to move to flat spacetime (where we use greek indices) and the objects we use in the second transformation I wrote down will be related to their corresponding curved space quantities using veirbeins?
 
  • #36
latentcorpse said:
so to summarise, the transformation in Minkowski space (the first one i wrote down) had latin indices because in Minkowski space we can define spinor transformations and this will hold in any basis so we can move to abstract indices.

However, in a curved spacetime we cannot define spinor transformations so we need to move to flat spacetime (where we use greek indices) and the objects we use in the second transformation I wrote down will be related to their corresponding curved space quantities using veirbeins?

Roughly correct. As far as the curved-space quantities, I can't see any reason why you would learn anything from transforming the local Lorentz transformation matrix into curved indices.
 
  • #37
This is beyond me...
 

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