SUMMARY
A representation ρ of a group G is always equivalent to a unitary representation on some inner product space V, particularly for finite groups. The inner product can be defined as <u, v> = (1/|G|) ∑g∈G <ρ(g)u, ρ(g)v>, which remains invariant under the action of the group. This principle extends to compact Lie groups, such as SO(3), where integration over the group can be applied to establish a similar inner product structure.
PREREQUISITES
- Understanding of group theory and representations
- Familiarity with inner product spaces
- Knowledge of compact Lie groups
- Basic concepts of invariant measures in mathematics
NEXT STEPS
- Study the proof of the equivalence of representations in "Representation Theory: A First Course" by Fulton and Harris
- Explore the properties of compact Lie groups in "Lie Groups, Lie Algebras, and Some of Their Applications" by Robert Gilmore
- Learn about the construction of invariant inner products in representation theory
- Research the specific representation theory of SO(3) in "Quantum Mechanics and Path Integrals" by Richard Feynman
USEFUL FOR
Mathematicians, physicists, and students studying representation theory, particularly those focusing on group representations and their applications in quantum mechanics and theoretical physics.