Definition

Let (π,H)(\pi,\mathcal H) be a of a group GG. A MHM\subseteq\mathcal H is invariant if

π(g)MMfor every gG.\pi(g)M\subseteq M\qquad\text{for every }g\in G.

Because g1Gg^{-1}\in G, this inclusion implies π(g)M=M\pi(g)M=M. Unitarity then makes the MM^\perp invariant as well, so MM is reducing and

H=MM\mathcal H=M\oplus M^\perp

is an orthogonal decomposition into subrepresentations.

Restricted representations

The restriction πM:GU(M)\pi|_M:G\to U(M) is again strongly continuous: each is the restriction of an orbit map in H\mathcal H. The PMP_M commutes with every π(g)\pi(g), and conversely a commuting orthogonal projection has invariant range. Thus invariant closed subspaces correspond exactly to orthogonal projections in the commutant of the representation.

Irreducibility and decomposition

The representation is irreducible when its only invariant closed subspaces are {0}\{0\} and H\mathcal H. Closedness matters in infinite dimension: an invariant dense proper does not contradict unitary irreducibility. Direct-sum and direct-integral decomposition theory studies representations through families of invariant closed subspaces and their associated projections Folland, §3.1.

Conventions and scope

For a single nonunitary operator or a semigroup representation, invariance of MM need not imply invariance of MM^\perp; then “invariant” and “reducing” are distinct. Their coincidence here uses both inverses in GG and the unitarity of every π(g)\pi(g).

References
  1. G. B. Folland, A Course in Abstract Harmonic Analysis, 2nd ed., CRC Press, 2016. DOI record. Relevant: §3.1 on invariant subspaces and irreducible unitary representations.