Microscopic shift asymptotics for zeta-derivative moments matching the CUE Kostka–determinant formula
Establish that for lists of non‑negative integers μ and ν of equal length s and fixed c ∈ ℂ, the mean value (1/T) ∫_{1}^{T} ∏_{i=1}^{s} ζ^{(μ_i)}(σ_T + i t) ∏_{j=1}^{s} overline{ζ^{(ν_j)}(σ_T + i t)} dt with σ_T = 1/2 + c / log T has leading-order asymptotics given by A_{μ,ν} (log T)^{|μ| + |ν| + s^2} times the universal coefficient μ! ν! ∑_{λ ⊢ |μ|, ℓ(λ) ≤ s} ∑_{ρ ⊢ |ν|, ℓ(ρ) ≤ s} K_{λ μ} K_{ρ ν} λ!_{(s)} ρ!_{(s)} det(I_{α_i(λ)+β_j(ρ)}(τ))_{i,j=1}^{s}, where α_i(λ)=λ_i + s − i, β_j(ρ)=ρ_j + s − j, τ = c + ar c, I_r(τ)=∫_{0}^{1} x^{r} e^{−τ x} dx, and A_{μ,ν} = ∏_{p} {(1 − p^{−1})^{s^2} ∑_{m=0}^{∞} (Γ(s+m)/(m! Γ(s)))^2 p^{−m}}.
References
Finally, it is reasonable to conjecture that the leading coefficients presented in Theorem \ref{thm:micro2} also arise from appropriately defined mean values of $\zeta$. Specifically, one expects that if the shifts on the left-hand side of eqn:ZetaMoments are taken to be $\sigma = \frac{1}{2}+\frac{c}{\log(T)}$, then the leading order asymptotics will be given by the random matrix result in climit, replacing $N$ with $\log(T)$ and multiplying by the arithmetic factor eqn:generalarithmetic.
eqn:ZetaMoments:
eqn:generalarithmetic: