Calculations of 239 Pu(n, F) prompt fission neutron spectra have been performed for neutron energy up to 20 MeV. The exclusive spectra of pre-fission neutron reactions (n, xnf) were calculated on the basis of the Hauser-Feshbach model simultaneously with the cross sections of (n, F) and (n, 2n) reactions. The spectra of neutrons emitted by fission fragments were approximated by a sum of two Watt distributions. The components of the prompt fission neutron spectra due to pre-fission neutrons are manifested in the prompt fission neutron spectra and the average neutron energy. A correlation is established between this effect in the contribution of emissive fission (n, xnf) in the fission cross-section of 239 Pu(n, F) and 235 U(n, F). It is shown that the 239 Pu(n, F) prompt fission neutron spectra used in applied calculations do not correspond to the experimental differential data and the systematic regularities in the spectra and their average energy found for the most carefully studied nuclei 235,238 U and 232 Th.The prompt fission neutron spectra of actinides have been investigated theoretically and experimentally from the moment the fission process was first discovered [1, 2]. Nevertheless, they have been investigated in detail only for 235 U and 238 U nuclei for neutron energy E n below and above the threshold for emissive fission, when together with the first chance fission reaction (n, f) the emissive fission reaction (n, xnf) with emission of x (≥ 1) neutrons is possible [3,4]. A decrease of the average energy of the spectrum of prompt fission neutrons near the threshold of the second chance fission reaction 235(238) U(n, nf) and the third chance fission reaction 235(238) U(n,2nf) has been investigated in detail experimentally [5,6].Pre-and post-fission neutrons contribute to the observed prompt fission neutron spectra at emissive fission excitation energies. This occurs when the energy E n of the neutrons is higher than E nnf , the threshold of the reaction (n, nf) (≈5-6 MeV). Post-fission prompt neutrons are emitted by primary fission fragments. Analysis of the spectra of prompt neutrons from the reactions 232 Th(n, f), 235 U(n, F), and 238 U(n, f) [here (n, F) denotes the sum of the reactions (n, f) and (n, xnf)] shows that many of their characteristic features can be correlated with the influence of pre-fission neutrons. For example, for E n > E n2nf the step features in the spectra of the prompt neutrons from the reactions 238 U(n, F) and 232 Th(n, F) at energy ε~ 3-5 MeV are due to the first neutron of the reaction (n, 2nf)-(n, 2nf) 1 [7-9]. The characteristic features of the shape of the spectra are also manifested for average energy 〈E〉; they are closely related with the chance (n, xnf) structure of the observed the fission cross-sections. This structure depends on the fissility of the nuclei (A + 1, Z), (A, Z), (A -1, Z), and so on, where (A, Z) is the target nucleus. Small-scale variations of the average energy were predicted for the reaction 232 Th(n, f) near the theshold of the reaction 232 Th(...