“…The first group includes the papers in which the nuclear excitations are treated as superposition of the one-particle-one-hole (1ph) configurations, that is within the RPA or the Tamm-Dancoff approximation (see, in particular, Refs. [3,4,[17][18][19][20][21][22][23][24]). In the papers of the second group, various versions of beyond-RPA approaches are used in which the RPA configuration space is enlarged by adding the 2ph, 1ph⊗phonon or two-phonons configurations (see, e.g., [25][26][27][28][29][30][31]).…”