Definition

Let FF be a , let GG be a connected , and write P=MNP=MN for a with MM and NN. For a (π,V)(\pi,V) of G(F)G(F), its unnormalized Jacquet module along PP is the N(F)N(F)-coinvariant space

VN=V/π(n)vv:nN(F), vV.V_N=V/\langle\pi(n)v-v:n\in N(F),\ v\in V\rangle.

It is naturally a smooth representation of M(F)M(F). The normalized Jacquet module is

rPG(V)=δP1/2VN,r_P^G(V)=\delta_P^{-1/2}\otimes V_N,

where δP\delta_P is the .

Adjointness

With compatible normalizations, iPGi_P^G is left adjoint to rPGr_P^G. Bernstein's second adjointness theorem gives rPGr_{\overline P}^G, for the opposite parabolic P\overline P, as a left adjoint to iPGi_P^G.

An irreducible is exactly when all of its Jacquet modules for proper parabolic subgroups vanish.

Exactness

Over complex coefficients the Jacquet functor is exact on smooth representations of a reductive pp-adic group. This is substantially stronger than arbitrary coinvariants and is one reason it is central to the structure theory of parabolic induction.

References
  1. I. N. Bernstein and A. V. Zelevinsky, “Induced representations of reductive pp-adic groups. I,” Annales scientifiques de l'École Normale Supérieure 10 (1977), 441–472. Numdam.
  2. William Casselman, “Introduction to the theory of admissible representations of pp-adic reductive groups,” unpublished notes, §4. UBC.