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Weyl Bounds for GL⁡2×GL⁡2\operatorname{GL}_2\times \operatorname{GL}_2 Rankin--Selberg LL-functions via Short Spectral Moments

Zihao Wang

Source record

Source: arXiv

Published: Oct 20, 2026

arXiv: 2610.27804

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Source abstract

Let ff and gg be Hecke--Maass cusp forms of SL⁡2(Z)\operatorname{SL}_2(\mathbb{Z}), with spectral parameters tft_f and tgt_g, respectively. Let TT be a large parameter and put L=∣T−tg∣.L = |T-t_g|. We prove the Lindelöf-on-average estimate ∑∣tf−T∣≤H∣L ⁣(12,f⊗g)∣2≪εT1+εH, \sum_{ |t_f-T|\leq H} \left|L\!\left(\frac12,f\otimes g\right)\right|^2 \ll_{\varepsilon} T^{1+\varepsilon}H, uniformly in the range T1/3+ε≪H,HTε≪L≤T. T^{1/3+\varepsilon}\ll H,\qquad HT^\varepsilon\ll L\leq T. As an immediate consequence, in the generic range when both ∣tg∣|t_g| and LL are of size TT, we obtain the Weyl bound L ⁣(12,f⊗g)≪εC(f×g)1/6+ε. L\!\left(\frac12,f\otimes g\right) \ll_\varepsilon C(f\times g)^{1/6+\varepsilon}.

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Weyl Bounds for $\operatorname{GL}_2\times \operatorname{GL}_2$ Rankin--Selberg $L$-functions via Short Spectral Moments — Mathematical Frontier Network