Questioning the 239Pu(n,2n)238Pu cross section shape above emission threshold

In the light of the JEF(F) European project longstanding story according to the determination of the most exact shape of the Pu(n, 2n)Pu reaction cross section and a recent measurement by Méot et al., this paper aims to shed another light on this topic by bringing new theoretical feedback. To achieve this goal, the AVXSF-LNG computer program has been upgraded to model second-chance reactions using its decay-probability module and, then chained to the TALYS-ECIS06 nuclear reaction system of codes. Present diligent calculation of the (n,2n) cross section over the energy range from the threshold to the onset of third-chance fission at about 12 MeV, suggests that current evaluations under-estimate the Pu(n,2n) cross section below 10 MeV; under-estimation of the order of 7% relatively to the JEFF-3.1 evaluation. On this ground, we propose an upward correction to the normalization of the measurement by Méot et al. Correction factor of about 1.24 with a maximum uncertainty on present fitted model estimated to ±11.6%. Latter value is extracted from a sensitivity analysis of the calculation route to the level density model that is selected for the non-equilibrated residual nucleus and to alternative choices we can make in terms of neutron fission cross section measurement references for the Pu and Pu target nuclei.