Chandee's conjecture on shifted moments of the Riemann zeta function

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Let k∈Nk\in\mathbb{N} and let α=(α1,α2){\bf\alpha}=(\alpha_1,\alpha_2) satisfy the hypotheses stated for the shifted moments: the shifts are real-valued functions of TT, are o(T)o(T), have the required limits involving αilog⁡T\alpha_i\log T and (αi−αj)log⁡T(\alpha_i-\alpha_j)\log T, and satisfy α1≠α2\alpha_1\ne\alpha_2 with α1−α2=O(1)\alpha_1-\alpha_2=O(1). Define

Ik(T,α1,α2)=∫0T∣ζ(12+i(t+α1))∣k∣ζ(12+i(t+α2))∣k dt.I_k(T,\alpha_1,\alpha_2)=\int_0^T\left|\zeta\left(\frac12+\mathrm{i}(t+\alpha_1)\right)\right|^k\left|\zeta\left(\frac12+\mathrm{i}(t+\alpha_2)\right)\right|^k\,dt.

Chandee's conjecture. One has

Ik(T,α1,α2){≍kT(log⁡T)k2,if lim⁡T→∞∣α1−α2∣log⁡T=0,≍k,cT(log⁡T)k2,if lim⁡T→∞∣α1−α2∣log⁡T=c≠0,≍kT(log⁡T∣α1−α2∣)k2/2,if lim⁡T→∞∣α1−α2∣log⁡T=∞.I_k(T,\alpha_1,\alpha_2)\begin{cases} \asymp_k T(\log T)^{k^2},&\text{if }\displaystyle\lim_{T\to\infty}|\alpha_1-\alpha_2|\log T=0,\\ \asymp_{k,c}T(\log T)^{k^2},&\text{if }\displaystyle\lim_{T\to\infty}|\alpha_1-\alpha_2|\log T=c\ne0,\\ \asymp_k T\left(\dfrac{\log T}{|\alpha_1-\alpha_2|}\right)^{k^2/2},&\text{if }\displaystyle\lim_{T\to\infty}|\alpha_1-\alpha_2|\log T=\infty. \end{cases}

This conjecture describes the transition in the size of two shifted zeta moments according to whether the shifts are closer than, comparable to, or farther apart than the scale 1/log⁡T1/\log T. It is presented as Chandee's conjecture based on the Keating–Snaith random matrix model; the paper proves related upper and lower bounds, but does not resolve the conjecture.

References

Primary source

Nathan Ng, Quanli Shen and Peng-Jie Wong, “Shifted moments of the Riemann zeta function”, arXiv:2206.03350 (2022).

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