“…In (1), N 1 and N 0 are the population densities of the levels 2p 5 3s3p LSJ and 2p 6 3s 2 S 1/2 , respectively, N e and v are the density and velocity of exciting electrons, σ 01 and σ 02 are the excitation crosssections from the ground states to the 2p 5 3s 2 2 P J0 and 2p 5 3s3p LSJ levels, respectively, A 10 and A a 1 are radiative and autoionization probabilities from the states 2p 5 3s 2 2 P J0 , respectively, and γ 21 is the fluorescence yield of the transition 2p 5 3s3p LSJ → 2p 5 3s 2 2 P J0 . The cross-sections for the excitation 2p 6 3s 2 S 1/2 → 2p 5 3s 2 2 P J0 are investigated both experimentally (e. g. [1,38]) and theoretically [38]. The excitation crosssections of the states 2p 5 3s3p LSJ were calculated in the present work by applying DW with exchange approximation.…”