We present a parametrization of the pair correlation function and the static structure factor of the Coulomb one component plasma (OCP) from the weakly coupled regime to the strongly coupled regime. Recent experiments strongly suggest that the OCP model can play the role of a reference system for warm dense matter. It can provide the ionic static structure factor that is necessary to interpret the x-ray Thomson scattering measurements, for instance. We illustrate this with the interpretation of a x-ray diffraction spectrum recently measured, using a Bayesian method that requires many evaluations of the static structure factor to automatically calibrate the parameters. For strongly coupled dusty plasmas, the proposed parametrization of the Coulomb OCP pair correlation function can be related to the Yukawa one, including screening. Further prospects to parametrize the static structure of Yukawa systems are also discussed.A realistic description of hot dense plasmas requires a model that includes all many-body interactions explicitly in contrast to weakly coupled plasmas that are well represented by only binary collisions and mean-field effects. This regime is characterized by strong interactions between ions, outweighing their thermal kinetic energy and leading to a liquid-like structure. Such strongly correlated plasmas are found in a variety of environments including planetary interiors, 1 dwarf stars, 2 and neutron star crusts 3 in astrophysics, and in many experimental set-ups of dusty plasmas, colloidal suspensions, 4 and warm dense matter (WDM) 5 in inertial confinement fusion studies. 6 Liquid metals 7 are also another manifestation of high Coulomb coupling in nature.In strongly coupled plasmas, the many-body interactions are not amenable to a theoretical approach in perturbation since there is no small parameters available. Besides very demanding state-of-the-art molecular dynamics simulations, a possible modeling comes through the definition of simpler idealized systems. These reference systems can be studied extensively by molecular dynamics once and for all, with results easily available through parametrizations and/or tabulations. The Coulomb 8,9 and Yukawa 10 one-component-plasma (OCP) systems are good candidates of such reference models.The Coulomb OCP represents a system of interacting ions, with the pair potential V C (r) = Qe/r, in a neutralizing uniform background of electrons. All its static and dynamic properties depend on only one parameter, the Coulomb coupling parameter Γ = Q 2 e 2 /ak B T , where Q is the ionic charge, T is the temperature, and a = (4πn/3) −1/3 is the Wigner-Seitz radius (n is the ionic density). The Coulomb coupling parameter Γ is a measure of the importance of correlation in plasmas as the ratio of the mean nearest neighbor interaction to the mean kinetic energy. The ideal gas-like behavior corresponds to Γ ≪ 1, liquid-like short-range order appears when Γ ≥ 1, and crystalline long-range order when Γ ≥ 180. Analytic parametrizations in Γ are available for the equation of ...