Refined Siegel–Weil conjecture for theta lifts

Let θΔ(τ,)\theta_{\Delta(\tau,\ell)} and θΔ(τ,2n+)\theta_{\Delta(\tau,2n+\ell)} be theta functions, and let Φ(θΔ(τ,),θΔ(τ,2n+),s)\Phi(\theta_{\Delta(\tau,\ell)},\theta_{\Delta(\tau,2n+\ell)},s) be the proposed section of ρΔ(τ,2n),s\rho_{\Delta(\tau,2n),s}. Let MsM_s and MsM_s^* be respectively the intertwining and normalized intertwining operators. Refined Siegel–Weil conjecture. For 1n1\leq\ell\leq n, the Eisenstein series attached to Φ(θΔ(τ,),θΔ(τ,2n+),s)\Phi(\theta_{\Delta(\tau,\ell)},\theta_{\Delta(\tau,2n+\ell)},s) is holomorphic at s=ns=\ell-n and, up to a possible constant, equals the theta integral at that point; moreover, the stated normalized-intertwining construction gives the residue identity in the intermediate case, while for n<2nn<\ell\leq2n the theta integral equals, up to a possible constant, the residue at s=ns=\ell-n:

Sp4(F)\Sp4(A)θΔ(τ,2n+)(g,h)θΔ(τ,)(g)dg=Values=nE(Φ(θΔ(τ,),θΔ(τ,2n+),s))(h)\int_{\operatorname{Sp}_{4\ell}(F)\backslash\operatorname{Sp}_{4\ell}(\mathbb A)}\theta_{\Delta(\tau,2n+\ell)}(g,h)\theta_{\Delta(\tau,\ell)}(g)\,dg=\operatorname{Value}_{s=\ell-n}E(\Phi(\theta_{\Delta(\tau,\ell)},\theta_{\Delta(\tau,2n+\ell)},s))(h)

when 1n1\leq\ell\leq n, with the additional intertwining assertion and residue formulation given in the source, and

Sp4(F)\Sp4(A)θΔ(τ,2n+)(g,h)θΔ(τ,)(g)dg=Ress=nE(Φ(θΔ(τ,),θΔ(τ,2n+),s))(h)\int_{\operatorname{Sp}_{4\ell}(F)\backslash\operatorname{Sp}_{4\ell}(\mathbb A)}\theta_{\Delta(\tau,2n+\ell)}(g,h)\theta_{\Delta(\tau,\ell)}(g)\,dg=\operatorname{Res}_{s=\ell-n}E(\Phi(\theta_{\Delta(\tau,\ell)},\theta_{\Delta(\tau,2n+\ell)},s))(h)

when n<2nn<\ell\leq2n. The corresponding normalized section is Φ=Ms(Φ)s=n\Phi^*=M_s^*(\Phi)|_{s=\ell-n} as specified in the source. This remains formal and is not established in the supplied context.

Sources & referencesView supporting material

Primary source

David Ginzburg and David Soudry, “A new regularized Siegel-Weil type formula, part I”, arXiv:2207.12818 (2022).

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