Exceptional-pole conjecture for GSp(4) × GL(2) L-factors

Let π\pi and σ\sigma be generic irreducible representations of GSp(4,F)\operatorname{GSp}(4,F) and GL(2,F)\operatorname{GL}(2,F), with central characters χπ\chi_{\pi} and χσ\chi_{\sigma}. Let s0Cs_0\in\mathbf C satisfy

χπχσ2s0=1.\chi_{\pi}\chi_{\sigma}|\cdot|^{2s_0}=1.

An exceptional pole is a pole in the exceptional part of Novodvorsky's local LL-factor.

Exceptional-pole conjecture. The point s0s_0 is an exceptional pole of L(π×σ,s)L(\pi\times\sigma,s) if and only if it is a pole of

L(π×σ,s)L(π×σ,s+1)L(π×σ×St,s+12).\frac{L(\pi\times\sigma,s)L(\pi\times\sigma,s+1)}{L(\pi\times\sigma\times\operatorname{St},s+\tfrac12)}.

Equivalently, the 88-dimensional Weil–Deligne representation ϕπϕσ\phi_{\pi}\otimes\phi_{\sigma} has a 11-dimensional unramified direct summand whose LL-factor has a pole at s0s_0. The conjecture gives a Langlands-parameter interpretation of exceptional poles; its general validity is not established in the source.

Sources & referencesView supporting material

Primary source

David Loeffler, “On local zeta-integrals for GSp(4) and GSp(4) x GL(2)”, arXiv:2011.15106 (2023).

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