“…Deformation was taken into account phenomenologically as in [22], by introducing the correction to ΔE de f C = ΔE sph C −δE de f C with the deformation parameters β 2 and β 4 from [23]. In the SU(4)-scheme, four types of ground states of nuclei belong to different supermultiplets: (i) (Z-even, N-even) nuclei belong to the (T Z , 0, 0) supermultiplet; (ii) (Z-even, N-odd) nuclei belong to the (T Z , 1/2, 1/2) supermultiplet; (iii) (Zodd, N-even) nuclei belong to the (T Z , 1/2, -1/2) supermultiplet; and (iv) (Z-odd, N-odd) nuclei belong to the (T Z , 1, 0) supermultiplet where the isospin T Z = (N − Z)/2.…”