The (σ,ρ)(\sigma,\rho)-Poisson summation formula

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Let kk be a number field, let GG be a kk-split reductive group, and let ρ ⁣:G∨(C)→GL⁡n(C)\rho\colon G^\vee(\mathbb{C})\to\operatorname{GL}_n(\mathbb{C}) be a finite-dimensional representation. For σ∈Acusp(G)\sigma\in\mathcal{A}_{\mathrm{cusp}}(G), let Sσ,ρ(A×)\mathcal{S}_{\sigma,\rho}(\mathbb{A}^\times) and Sσ~,ρ(A×)\mathcal{S}_{\widetilde{\sigma},\rho}(\mathbb{A}^\times) be the associated Schwartz spaces, let Fσ,ρ,ψ\mathcal{F}_{\sigma,\rho,\psi} be the associated Fourier operator, and write Θσ,ρ(x,ϕ)=∑α∈k×ϕ(αx)\Theta_{\sigma,\rho}(x,\phi)=\sum_{\alpha\in k^\times}\phi(\alpha x). Then there exist k×k^\times-invariant linear functionals Eσ,ρ\mathcal{E}_{\sigma,\rho} and Eσ~,ρ\mathcal{E}_{\widetilde{\sigma},\rho} on the respective Schwartz spaces such that (σ,ρ)(\sigma,\rho)-Poisson summation formula.

Eσ,ρ(ϕ)=Eσ~,ρ(Fσ,ρ,ψ(ϕ))\mathcal{E}_{\sigma,\rho}(\phi)=\mathcal{E}_{\widetilde{\sigma},\rho}(\mathcal{F}_{\sigma,\rho,\psi}(\phi))

for every ϕ∈Sσ,ρ(A×)\phi\in\mathcal{S}_{\sigma,\rho}(\mathbb{A}^\times). Moreover, if ϕ∈Sσ,ρ∘∘(A×)\phi\in\mathcal{S}_{\sigma,\rho}^{\circ\circ}(\mathbb{A}^\times), then

Eσ,ρ(ϕx)=Θσ,ρ(x,ϕ)=∑α∈k×ϕ(αx),\mathcal{E}_{\sigma,\rho}(\phi^x)=\Theta_{\sigma,\rho}(x,\phi)=\sum_{\alpha\in k^\times}\phi(\alpha x),

where ϕx(⋅)=ϕ(⋅x)\phi^x(\cdot)=\phi(\cdot x) for x∈A×x\in\mathbb{A}^\times. This is the conjectural global Poisson summation formula underlying the proposed Fourier analysis on GL1\mathrm{GL}_1 and the associated automorphic LL-functions; its status is not resolved in the supplied source.

References

Primary source

Dihua Jiang and Zhilin Luo, “Certain Fourier Operators on GL_1 and Local Langlands Gamma functions”, arXiv:2108.03565 (2022).

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