Definition

Let G=G(F)G=\mathbf G(F) for a connected over a , let P=MNP=MN be a with MM and NN, and let σ\sigma be a of MM, inflated across NN. The normalized parabolic induction is

iPG(σ)=IndPG(δP1/2σ),i_P^G(\sigma)=\operatorname{Ind}_P^G \bigl(\delta_P^{1/2}\otimes\sigma\bigr),

where δP\delta_P is the . The half-modulus factor makes induction carry unitary representations to unitary representations.

Function model

In the right-equivariant convention, the representation consists of locally constant functions f:GVσf:G\to V_\sigma, with the usual support condition modulo PP, satisfying

f(gmn)=δP(m)1/2σ(m)1f(g).f(gmn)=\delta_P(m)^{-1/2}\sigma(m)^{-1}f(g).

The group GG acts by .

Role in the Langlands classification

The says that every irreducible admissible representation is the unique irreducible quotient of iPG(τχ)i_P^G(\tau\otimes\chi) for suitable τ\tau on a Levi subgroup and a character χ\chi in a positive chamber. provide the primitive inducing data further down the classification.

Convention warning

Some authors build the factor δP1/2\delta_P^{1/2} into the symbol Ind\operatorname{Ind}, while others call that functor unnormalized induction. Left-versus-right equivariance also reverses the displayed power. The invariant content is the half-density correction.

References
  1. Joseph Bernstein and Andrei Zelevinsky, “Induced representations of reductive pp-adic groups I,” Annales scientifiques de l’École Normale Supérieure 10 (1977), 441–472. Numdam.
  2. Tasho Kaletha, “Representations of reductive groups over local fields,” §1, 2022. arXiv.