Why complex reps of gauge group for chiral theory?

In summary, the gauge group must be in a complex representation for the fermions to exhibit chirality, which is defined as the property of being left-handed Weyl spinors. This is different from the chirality matrix γ5 which determines handedness of fermions. For a theory to be chiral, fermions must be massless and come in complex representations of the gauge group. This is not the case in QCD, as the quarks are massive and do not come in complex representations. Therefore, QCD is considered a non-chiral theory.
  • #1
Lapidus
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Why must the gauge group be in a complex representation so that chirality of the fermions is respected?

thanks
 
  • #3
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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  • #4
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.
 

1. Why do we need complex representations of gauge groups in chiral theories?

Complex representations are necessary for chiral theories because they allow for the existence of chiral fermions, which are particles that have a different left-handed and right-handed behavior. This is important because it explains why certain particles, such as neutrinos, only interact with one type of weak nuclear force. Real representations do not allow for this type of behavior.

2. How do complex representations change the behavior of gauge theories?

Complex representations introduce a new mathematical structure called a complex gauge group, which can be thought of as a combination of a real gauge group and a complex phase factor. This allows for the possibility of chiral interactions and explains why certain particles have different interactions with the weak nuclear force.

3. Are there any other benefits of using complex representations in gauge theories?

Yes, complex representations also allow for the unification of the weak and electromagnetic forces. This is because the complex gauge group structure allows for the mixing of these two forces, which is observed in nature. This unification is a key aspect of the Standard Model of particle physics.

4. Can chiral theories be described using only real representations?

No, chiral theories require the use of complex representations as they cannot be fully described using only real representations. Real representations do not allow for the existence of chiral particles and cannot fully explain the observed behavior of particles in the weak nuclear force.

5. How do complex representations affect the symmetry of gauge theories?

Complex representations introduce a new type of symmetry called chiral symmetry, which is necessary for the existence of chiral fermions. This symmetry is different from the usual gauge symmetry and plays a crucial role in explaining the behavior of particles in chiral theories.

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