Any electronic eigenstate of the paramagnetic ion open-shell is characterized by the three independent multipole asphericities for and 6 related to the second moments of the relevant crystal-field splittings byThe A k as the reduced matrix elements can serve as a reliable measure of the state capability for the splitting produced by the k-rank component of the crystal-field Hamiltonian. These multipolar characteristics allow one to verify any fitted crystal-field parameter set by comparing the calculated second moments and the experimental ones of the relevant crystal-field splittings. We present the multipole characteristics A k for the extensive set of eigenstates from the lower parts of energy spectra of the tripositive 4 f N ions applying in the calculations the improved eigenfunctions of the free lanthanide ions obtained based on the M. Reid f-shell programs. Such amended asphericities are compared with those achieved for the simplified Russell-Saunders states. Next, they are classified with respect to the absolute or relative weight of A k in the multipole structure of the considered states. For the majority of the analyzed states (about 80%) the A k variation is of order of only a few percent. Some essential changes are found primarily for several states of Tm 3+ , Er 3+ , Nd 3+ , and Pr 3+ ions. The detailed mechanisms of such A k changes are unveiled. Particularly, certain noteworthy cancelations as well as enhancements of their magnitudes are explained.