“…In the case of one-photon transitions (p = 1) within the configuration nℓ N , (20) with k S = 0 gives as a special case the operator implicitly considered by several people in order to explain intra-configurational one-photon transitions for d N [1,2] or f N [3,4] ions in crystals. In the case of inter-configurational two-photon transitions (p = 2) between the configuration nℓ N and the configuration nℓ N−1 n ′ ℓ ′ with ℓ + ℓ ′ odd, (20) with k S = 0 yields as particular cases the operators introduced in connection with either a static coupling mechanism [13,16,19,22,24] when X (t) is the odd crystal-field tensor or a dynamic coupling mechanism [19,22] when X (t) is the ligand polarization tensor.…”