SUMMARY
The charge associated with the weak interaction is defined by two components: weak isospin and weak hypercharge, which arise from the electroweak theory represented by the symmetry group SU(2)xU(1). Weak isospin is the SU(2) charge, while weak hypercharge is analogous to electric charge in electromagnetism, with particles possessing either positive or negative values. The mediating particles for these interactions are the W and Z bosons, with the Z boson being a combination of the third component of weak isospin and hypercharge. Right-handed fermions do not carry weak isospin charge.
PREREQUISITES
- Understanding of electroweak theory and its symmetry group SU(2)xU(1)
- Familiarity with particle physics terminology, including weak isospin and weak hypercharge
- Knowledge of gauge bosons, specifically W and Z bosons
- Basic concepts of quantum field theory and particle interactions
NEXT STEPS
- Study the electroweak unification and its implications in particle physics
- Learn about the role of gauge symmetries in quantum field theory
- Explore the properties and interactions of W and Z bosons
- Investigate the differences between weak isospin and isospin in particle physics
USEFUL FOR
Physicists, students of particle physics, and anyone interested in the fundamental interactions of particles and the structure of the Standard Model.