Ichino–Ikeda refinement of the global Gross–Prasad conjecture

Let FF, A\mathbb{A}, VnV_n, Vn+1V_{n+1}, SOn\operatorname{SO}_n, and SOn+1\operatorname{SO}_{n+1} be as above, and let P(ϕ,f)=SOn(F)\SOn(A)ϕ(g)f(g)dg\mathcal{P}(\phi,f)=\int_{\operatorname{SO}_n(F)\backslash\operatorname{SO}_n(\mathbb{A})}\phi(g)f(g)\,dg. For factorizable vectors, write ϕ=vϕv\phi=\otimes_v\phi_v and f=vfvf=\otimes_v f_v, and let αv(ϕv,fv)\alpha_v(\phi_v,f_v) denote the normalized local period. Ichino–Ikeda refinement. Assume that πn+1\pi_{n+1} and πn\pi_n are tempered cuspidal automorphic representations of SOn+1(A)\operatorname{SO}_{n+1}(\mathbb{A}) and SOn(A)\operatorname{SO}_n(\mathbb{A}), respectively, and appear with multiplicity one in the discrete spectrum. Then

P(ϕ,f)2=ΔSOn+12βL(1/2,πn×πn+1)L(1,πn,Ad)L(1,πn+1,Ad)vαv(ϕv,fv),|\mathcal{P}(\phi,f)|^2=\frac{\Delta_{\operatorname{SO}_{n+1}}}{2^\beta}\frac{L(1/2,\pi_n\times\pi_{n+1})}{L(1,\pi_n,\operatorname{Ad})L(1,\pi_{n+1},\operatorname{Ad})}\prod_v\alpha_v(\phi_v,f_v),

where 2β2^\beta is the product of the cardinalities of the component groups attached to the LL-packets, and ΔSOn+1\Delta_{\operatorname{SO}_{n+1}} is defined by the parity of dimVn+1\dim V_{n+1} as in the source. The conjecture refines the nonvanishing criterion by predicting the exact normalized period formula.

Sources & referencesView supporting material

Primary source

Melissa Emory, “On the global Gan-Gross-Prasad conjecture for general spin groups”, arXiv:1901.01746 (2019).

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