SUMMARY
The SU(3) defining representation decomposes into an SU(2) doublet with hypercharge (1/3) and a singlet with hypercharge (-2/3). This decomposition is achieved by utilizing block diagonal forms or tensor products of the fundamental representation, employing Young tableaux methods. The representation remains valid under the SU(2) x U(1) subgroup, as elements are mapped accordingly. Understanding this process is facilitated by selecting a basis where SU(2) is generated by the Gell-Mann matrices λ1, λ2, λ3, and U(1) by λ8.
PREREQUISITES
- Understanding of SU(3) and its defining representation
- Familiarity with SU(2) and U(1) groups
- Knowledge of Gell-Mann matrices and their properties
- Experience with Young tableaux methods for representation theory
NEXT STEPS
- Study the decomposition of representations in Lie algebras
- Learn about the application of Young tableaux in representation theory
- Explore Tinkham's "Group Theory and Quantum Mechanics" for additional insights
- Investigate the relationship between Pauli matrices and SU(2) subgroups
USEFUL FOR
The discussion is beneficial for theoretical physicists, particle physicists, and students of quantum mechanics who are exploring representation theory in the context of gauge groups.