Definition

For a ρ:GGL(V)\rho:G\to\operatorname{GL}(V), the fixed-vector subspace, or space of invariants, is

VG={vV:ρ(g)v=v for every gG}.V^G=\{v\in V:\rho(g)v=v\text{ for every }g\in G\}.

For a dρ:ggl(V)d\rho:\mathfrak g\to\mathfrak{gl}(V), it is

Vg={vV:dρ(X)v=0 for every Xg}.V^{\mathfrak g}=\{v\in V:d\rho(X)v=0\text{ for every }X\in\mathfrak g\}.

Both are linear subspaces and subrepresentations carrying the trivial action.

Universal description

The fixed space can be written as an intersection of kernels,

VG=gGker(ρ(g)I),Vg=Xgker(dρ(X)).V^G=\bigcap_{g\in G}\ker(\rho(g)-I), \qquad V^{\mathfrak g}=\bigcap_{X\in\mathfrak g}\ker(d\rho(X)).

Equivalently, VGV^G is naturally the space HomG(1,V)\operatorname{Hom}_G(\mathbf1,V) of from the trivial one-dimensional representation. Thus dimVG\dim V^G is the of the trivial representation whenever VV is completely reducible.

Compact-group averaging

If GG is compact and VV is a continuous finite-dimensional representation, normalized defines the Reynolds projection

P(v)=Gρ(g)vdg.P(v)=\int_G\rho(g)v\,dg.

It satisfies P2=PP^2=P and imP=VG\operatorname{im}P=V^G. This turns the abstract invariant subspace into a computable direct summand.

Group versus Lie algebra

Every group-fixed vector is fixed infinitesimally. If GG is connected, then

VG=Vg.V^G=V^{\mathfrak g}.

For disconnected GG, the equality can fail because VgV^{\mathfrak g} only records invariance under the . The remaining component group may act nontrivially on VgV^{\mathfrak g}.

The term “invariant vector” means a fixed vector. It should not be confused with an invariant subspace, whose individual vectors may move within that subspace.

References
  1. Brian C. Hall, Lie Groups, Lie Algebras, and Representations, 2nd ed., Springer, 2015, Chapters 4 and 11. Publisher record.
  2. Anthony W. Knapp, Lie Groups Beyond an Introduction, 2nd ed., Birkhäuser, 2002, Chapter IV. Publisher record.