The global numerical conjecture for polarized hyperspherical Hamiltonian varieties

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Let M=T∗XM=T^*X and Mˇ=T∗Xˇ\check{M}=T^*\check{X} be a pair of dual polarized hyperspherical Hamiltonian varieties, where XX is a GG-spherical variety and Xˇ\check{X} is the corresponding Gˇ\check{G}-spherical variety. Let π\pi be a tempered automorphic representation of G(A)G(\mathbb{A}) with LL-parameter ϕ\phi. Suppose that the fixed point set

Xˇϕ={x1,…,xr}\check{X}^{\phi}=\{x_1,\dots,x_r\}

is finite. For a suitably normalized spherical vector f∈πf\in\pi, The global numerical conjecture. one has

PX(f)∼∑i=1rL(0,(TxiXˇ)\talloblong).\mathcal{P}_X(f)\sim \sum_{i=1}^rL(0,(T_{x_i}\check{X})^{\talloblong}).

Here ∼\sim suppresses the global constants and local factors at ramified places occurring in a precise period formula. This is the expected numerical relation between the automorphic period attached to XX and special values of LL-functions associated with the fixed points of the Langlands parameter on the dual variety; the precise global period formula, including its constants and ramified local factors, remains to be established in this setting.

References

Primary source

Shenghao Li, “Bump-Friedberg type periods beyond the cuspidal spectrum”, arXiv:2607.10289 (2026).

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