The commuting direction in solution provides the correct candidate Lie algebra for a gauge group, . This is a necessary structural condition for the Standard Model, but it does not by itself establish a viable grand unified theory.
The representations in solution do not give a Standard Model fermion generation with the correct weak hypercharges. Use . Identifying with the left-handed quark doublet, whose weak hypercharge is , fixes . But then the doublet in has , whereas the left-handed lepton doublet requires . Its singlet has , whereas a right-handed electron requires . The is a further concrete mismatch: right-handed quarks written as left-handed antiquarks require or , and a rescaling cannot turn zero into either value. These comparisons use the electroweak representation and hypercharge table.
The charge- doublet in does have the required lepton weak hypercharge under this normalization, but the same Adjoint representation also brings a doublet of the opposite charge and an extra triplet. Therefore merely adding that representation does not supply the missing chiral generation without additional states and a mechanism for their masses.
Furthermore is a product of two Simple Lie groups, permitting two independent gauge couplings; it does not enforce a common strong and electroweak gauge coupling. Thus the embedding exists, but the displayed matter content does not furnish a viable minimal unification of the Standard Model. A more elaborate model would require additional representations, consistent chiral matter, anomaly cancellation, and a specified spontaneous symmetry breaking mechanism. The calculations here do not prove that every possible extension using this product group is impossible.

Articles by others on the same topic (0)

There are currently no matching articles.