“…More precisely, the configuration sets explicitly retained for the computations were 4f 12 , 4f 11 6p, 4f 11 7p, 4f 11 5f, 4f 11 6f for the even parity, and 4f 11 6s, 4f 11 7s, 4f 11 5d, 4f 11 6d, 4f 11 7d for the odd parity. The core-valence interactions were included by means of a core-polarization pseudo-potential and a correction to the dipole operator according to the procedure described in many of our previous papers (see e.g., [25][26][27]). As a reminder, for atomic systems with n valence electrons, this core-polarization potential gives rise to the following one-particle, V P1 , and two-particle, V P2 , contributions:…”