Why complex reps of gauge group for chiral theory?

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SUMMARY

The discussion clarifies that for a theory to be chiral, fermions must be massless Weyl spinors and exist in complex representations of the gauge group. Specifically, the standard model fermions are conventionally defined as left-handed Weyl spinors, which are massless and respect chirality. In contrast, Quantum Chromodynamics (QCD) features complex representations, such as the fundamental representation of the color gauge group SU(3), but does not qualify as a chiral theory due to the presence of massive quarks that are not chirality eigenstates.

PREREQUISITES
  • Understanding of Weyl spinors and their properties
  • Familiarity with gauge groups, specifically SU(3) and the Standard Model group
  • Knowledge of chirality and chirality matrices, particularly γ5
  • Basic concepts of Quantum Chromodynamics (QCD)
NEXT STEPS
  • Study the properties of Weyl spinors in quantum field theory
  • Research the implications of complex representations in gauge theories
  • Explore the role of chirality in the Standard Model of particle physics
  • Examine the differences between chiral and non-chiral theories in particle physics
USEFUL FOR

The discussion is beneficial for theoretical physicists, particle physicists, and students studying quantum field theory, particularly those interested in the properties of fermions and gauge theories.

Lapidus
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Why must the gauge group be in a complex representation so that chirality of the fermions is respected?

thanks
 
Lapidus said:
Why must the gauge group be in a complex representation so that chirality of the fermions is respected?

thanks
I think your confusion is a matter of semantics or definition/convention. By convention all standard model fermions are taken to be left handed weyl spinors i.e. massless. Then property that these massless Weyl fermions are in a complex representation of the standard model group is called or defined to be "chirality". Not to be confused with chirality matrix γ5 which determines handedness chirality of fermions. Chiral (handedness eigenstates) fermions when appear in complex representations of the gauge group makes the THEORY chiral.
Recall in QCD, we also have complex representations, e.g. fundamental of color gauge group SU(3). But this does NOT make QCD a chiral theory because the quarks/fermions being massive are not chirality eigenstates i.e. constituents are not chiral fermions.

So we need 2 things for a theory to be chiral, a) fermions must be massless, ie. chiral fermions b) they should come in complex representations of the gauge group.
 
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Roy_1981 said:
al.
Recall in QCD, we also have complex representations, e.g. fundamental of color gauge group SU(3). But this does NOT make QCD a chiral theory

In fact there is a bit of Doctrine here, as we could equally define that QCD is non-chiral SU(3), similar to electromagnetism in this aspect.
 

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