Frequency moments of the Coulomb dynamic structure factor and related integrals

This report addresses the moments, ${\mathfrak{G}n}\left( {$\mathbf{q}$} \right) = \int{ - \infty }^{ + \infty } {{\omega ^n}S\left( {{$\mathbf{q}$},\omega } \right)$\mathrm{d}$\omega },,n \in $\mathbb{N}$,,n \geq - 1$,ofthequantummechanicaldynamicstructurefactor$S\left( {{$\mathbf{q}$},\omega } \right)$ for a one-component Coulomb plasma in thermodynamic equilibrium. The Fluctuation Dissipation Theorem relates these moments to integrals involving the imaginary part of the inverse longitudinal dielectric function, with the odd moments in particular being equivalent to the odd moments of the imaginary part of the inverse dielectric function. Application of the Generalized Plasmon Pole Approximation arXiv:1508.05606 [physics.plasm-ph] to a weakly-coupled non-degenerate plasma, leads to general formulae expressed in terms of polynomial functions. Explicit forms of these functions are given for $n\le 20$. These formulae are generalized to degenerate and partially degenerate plasmas, in small-$\mathbf{q}$ (long-wavelength) regimes.