Q&A on String Theory Course Indices/QFT

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SUMMARY

This discussion focuses on advanced topics in string theory and quantum field theory (QFT), specifically regarding the manipulation of Dirac spinors and the properties of gamma matrices. Key points include the definition of spinor indices, the implications of transposing products of anticommuting objects, and the relationship between the transpose and Hermitian conjugate operations. The participants clarify that the Polyakov action describes a bosonic string and address the implications of equations of motion for left-moving waves.

PREREQUISITES
  • Understanding of Dirac spinors and their indices in quantum field theory.
  • Familiarity with gamma matrices and their role in representing spinor transformations.
  • Knowledge of Grassmann algebra and properties of anticommuting variables.
  • Basic concepts of the Polyakov action in string theory.
NEXT STEPS
  • Study the properties of Dirac spinors and their indices in detail.
  • Learn about the implications of Grassmann parity in quantum field theory.
  • Explore the derivation and applications of the Polyakov action in string theory.
  • Investigate the relationship between Hermitian conjugates and transpositions in the context of anticommuting variables.
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Students and researchers in theoretical physics, particularly those focusing on string theory, quantum field theory, and the mathematical foundations of particle physics.

  • #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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