Definition

Let a GG act measurably on a standard Borel space XX. A system of imprimitivity for this action on a complex H\mathcal H is a pair (U,P)(U,P), where UU is a of GG on H\mathcal H and PP is a on XX, such that

U(g)P(E)U(g)1=P(gE)U(g)P(E)U(g)^{-1}=P(gE)

for every gGg\in G and every Borel set EXE\subseteq X. The equation is the covariance axiom linking the representation to the action on measurable subsets.

Function-algebra formulation

Integrating bounded against PP gives a representation MPM_P by operators on H\mathcal H. Covariance becomes

U(g)MP(f)U(g)1=MP(fg1).U(g)M_P(f)U(g)^{-1}=M_P(f\circ g^{-1}).

Thus a system of imprimitivity can equivalently be viewed as a covariant representation of the action on functions. The projection-valued and function-algebra formulations contain the same information.

Transitive actions and induction

When X=G/HX=G/H is a ]] for a closed subgroup HH, Mackey's classifies systems based on G/HG/H by unitary representations of HH. The associated representation of GG is induced from HH, and P(E)P(E) acts by multiplication by the indicator of EE. This equivalence is the main bridge between induction and spectral localization Mackey, pp. 537–545.

Examples and non-examples

For the translation action of GG on itself, let H=L2(G)\mathcal H=L^2(G), let UU be the , and let P(E)P(E) multiply by 1E1_E. This is a system of imprimitivity. Pairing the same PP with a representation that does not transport supports according to the action fails the covariance axiom.

References
  1. George W. Mackey, “Imprimitivity for Representations of Locally Compact Groups I,” Proceedings of the National Academy of Sciences 35 (1949), 537–545. DOI record. Relevant: the transitive imprimitivity theorem.
  2. Gerald B. Folland, A Course in Abstract Harmonic Analysis, 2nd ed., CRC Press, 2016. DOI record. Relevant: §6.3, systems of imprimitivity and induced representations.