Let π:G→U(H)\pi:G\to U(H) be a on a nonzero . It is irreducible if its only are {0}\{0\} and HH. Closedness is essential in infinite-dimensional Hilbert spaces: the definition is topological, not purely algebraic. Because every π(g)\pi(g) is unitary and π(g)−1=π(g−1)\pi(g)^{-1}=\pi(g^{-1}), a closed invariant subspace is automatically reducing, so its is invariant as well.

Commutant characterization

The representation is irreducible if and only if every bounded operator TT satisfying Tπ(g)=π(g)TT\pi(g)=\pi(g)T for all g∈Gg\in G is a scalar multiple of the identity. Equivalently, the of π(G)\pi(G) is CI\mathbb C I. This is the unitary form of . A nontrivial invariant subspace yields a nonscalar commuting , while the spectral projections of a nonscalar self-adjoint operator in the commutant recover a nontrivial invariant subspace.

Examples and reducible cases

Every one-dimensional unitary representation is irreducible. The trivial representation on C\mathbb C is the simplest example. A nontrivial orthogonal direct sum π1⊕π2\pi_1\oplus\pi_2 is reducible because each summand is a proper closed invariant subspace. An cannot have two orthogonal nonzero invariant summands.

Conventions and scope

Noncompactness does not force irreducible unitary representations to be infinite-dimensional. For instance, R×SU⁡(2)\mathbb R\times\operatorname{SU}(2) has the (t,k)↦eitk(t,k)\mapsto e^{it}k. Conversely, topological irreducibility on a Hilbert space does not imply algebraic irreducibility of the .

References
  1. Gerald B. Folland, A Course in Abstract Harmonic Analysis, 2nd ed., CRC Press, 2016. DOI record. Relevant: §3.1 on invariant subspaces, irreducibility, and Schur's lemma.