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