SUMMARY
The discussion centers on the projective representations of the spin group, specifically addressing why projective representations of Spin(n) are not considered in quantum mechanics (QM). It concludes that for n>2, Spin(n) serves as a universal cover, allowing for the redefinition of operator phases, resulting in no nontrivial projective representations. For n=1 and n=2, the analysis indicates that these cases involve anyons and that the projective representations of SU(2) are trivially related to its linear representations due to the semi-simple nature of its Lie algebra.
PREREQUISITES
- Understanding of projective representations in group theory
- Familiarity with Spin(n) and its relationship to SO(n)
- Knowledge of Lie algebras and their central extensions
- Basic concepts of quantum mechanics, particularly spinors
NEXT STEPS
- Study the properties of projective representations in group theory
- Explore the relationship between Spin(n) and SO(n) in detail
- Investigate the implications of central extensions in Lie algebras
- Learn about anyons and their role in quantum mechanics
USEFUL FOR
The discussion is beneficial for theoretical physicists, mathematicians specializing in group theory, and quantum mechanics researchers focusing on spinor representations and their implications in particle physics.