Refined Siegel–Weil conjecture for theta lifts

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Let θΔ(τ,ℓ)\theta_{\Delta(\tau,\ell)} and θΔ(τ,2n+ℓ)\theta_{\Delta(\tau,2n+\ell)} be theta functions, and let Φ(θΔ(τ,ℓ),θΔ(τ,2n+ℓ),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 Ms∗M_s^* be respectively the intertwining and normalized intertwining operators. Refined Siegel–Weil conjecture. For 1≤ℓ≤n1\leq\ell\leq n, the Eisenstein series attached to Φ(θΔ(τ,ℓ),θΔ(τ,2n+ℓ),s)\Phi(\theta_{\Delta(\tau,\ell)},\theta_{\Delta(\tau,2n+\ell)},s) is holomorphic at s=ℓ−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<ℓ≤2nn<\ell\leq2n the theta integral equals, up to a possible constant, the residue at s=ℓ−ns=\ell-n:

∫Sp⁡4ℓ(F)\Sp⁡4ℓ(A)θΔ(τ,2n+ℓ)(g,h)θΔ(τ,ℓ)(g) dg=Value⁡s=ℓ−nE(Φ(θΔ(τ,ℓ),θΔ(τ,2n+ℓ),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 1≤ℓ≤n1\leq\ell\leq n, with the additional intertwining assertion and residue formulation given in the source, and

∫Sp⁡4ℓ(F)\Sp⁡4ℓ(A)θΔ(τ,2n+ℓ)(g,h)θΔ(τ,ℓ)(g) dg=Res⁡s=ℓ−nE(Φ(θΔ(τ,ℓ),θΔ(τ,2n+ℓ),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<ℓ≤2nn<\ell\leq2n. The corresponding normalized section is Φ∗=Ms∗(Φ)∣s=ℓ−n\Phi^*=M_s^*(\Phi)|_{s=\ell-n} as specified in the source. This remains formal and is not established in the supplied context.

References

Primary source

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

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