Joint Gaussian value distribution conjecture for orthogonal Hecke–Maass cusp forms

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Let J≥2J\geq2, and let fjf_j, 1≤j≤J1\leq j\leq J, be pairwise orthogonal real-valued Hecke–Maass cusp forms for SL⁡2(Z)\operatorname{SL}_2(\mathbb{Z}), with spectral parameters tfjt_{f_j}. Assume

1vol⁡(Γ\H)∫Γ\H∣fj(z)∣2 dμz=1,1≤j≤J.\frac{1}{\operatorname{vol}(\Gamma\backslash\mathbb{H})}\int_{\Gamma\backslash\mathbb{H}}|f_j(z)|^2\,\mathrm{d}\mu z=1,\qquad 1\leq j\leq J.

Let aja_j be positive integers. Joint Gaussian value distribution conjecture. The powers {fjaj}j=1J\{f_j^{a_j}\}_{j=1}^J are statistically independent: for every ψ∈Cc∞(Γ\H)\psi\in\mathcal{C}_c^\infty(\Gamma\backslash\mathbb{H}),

∫Γ\Hψ(z)∏j=1Jfj(z)aj dμz=(∏j=1Jcaj)∫Γ\Hψ(z) dμz+o(1)\int_{\Gamma\backslash\mathbb{H}}\psi(z)\prod_{j=1}^J f_j(z)^{a_j}\,\mathrm{d}\mu z=\left(\prod_{j=1}^Jc_{a_j}\right)\int_{\Gamma\backslash\mathbb{H}}\psi(z)\,\mathrm{d}\mu z+o(1)

as min⁡(tf1,…,tfJ)→∞\min(t_{f_1},\ldots,t_{f_J})\to\infty, where ca=(2a−1)!!c_a=(2a-1)!! for even aa and ca=0c_a=0 for odd aa. This predicts that distinct orthogonal Hecke–Maass cusp forms behave like independent random waves in the semiclassical limit. The paper proves two conditional joint-moment results supporting the conjecture, but the full assertion remains open.

References

Primary source

Shenghao Hua, Bingrong Huang and Liangxun Li, “Joint value distribution of Hecke–Maass forms”, arXiv:2405.00996 (2024).

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