“…Through this one defines the function J ω ϕ ℓ,q (ν V , p V ) : G → C when (ν V , p V ) are the spectral parameters of an arbitrary irreducible subspace V ⊂ 0 L 2 (Γ\G). As noted in [22,Subsection 1.7] (see, in particular, [22,Relations (1.7.10) and (1.5.17)]), each term F c ω f in the Fourier expansion at any cusp c of any function f ∈ V K,ℓ,q is a constant multiple of the corresponding Jacquet integral, J ω ϕ ℓ,q (ν V , p V ) : G → C. Indeed, it is even possible to choose, for the subspace factors V K,ℓ,q in (1.1.5), a system of generators,…”