“…The first method used for modeling the atomic structure and computing the radiative parameters in Lu V was the pseudo-relativistic Hartree-Fock (HFR) approach developed by Cowan [5], using the suite of codes RCN, RCN2 and RCG adapted by the Atomic Physics and Astrophysics group of Mons University for the atomic structure calculations in heavy elements [13]. Configuration interaction was considered by explicitly including in the calculations the 4f 13 , 4f 12 6p, 4f 12 7p, 4f 12 8p, 4f 12 5f, 4f 12 6f, 4f 12 7f, 4f 12 8f, 4f 11 5d 2 , 4f 11 6s 2 , 4f 11 6p 2 , 4f 11 5d6s, 5p 5 4f 14 , 5p 5 4f 13 6p odd-parity configurations, and the 4f 12 6s, 4f 12 7s, 4f 12 8s, 4f 12 5d, 4f 12 6d, 4f 12 7d, 4f 12 8d, 4f 12 5g, 4f 12 6g, 4f 12 7g, 4f 12 8g, 4f 11 6s6p, 4f 11 5d6p, 5p 5 4f 13 6s and 5p 5 4f 13 5d even-parity configurations. These configurations represent the majority of those lying (and overlapping) below the Lu V ionization potential, as shown in Figures 2 and 3, where their energy ranges, estimated from Monoconfigurational HFR calculations, are plotted for odd and even parities, respectively.…”