Abstract

The high-order perturbation formulas of spin-Hamiltonian (SH) parameters ( g factors g ∥, g ⊥ and zero-field splitting D) for 3d 8 ions in trigonal octahedral sites of crystals are derived considering not only the crystal-field (CF) mechanism, but also the charge-transfer (CT) mechanism (which is neglected in the extensively used CF theory). From these formulas and by considering the suitable impurity-induced local lattice relaxation, the SH parameters of CsCdX 3:Ni 2+ (X = Cl, Br) crystals are calculated. The results are in reasonable agreement with the experimental values. The sign of Q CT ( Q = Δ g ∥, Δ g ⊥ or D, where the g-shift Δ g i = g i − g e, g e ≈ 2.0023 is the free-electron value) due to CT mechanism is the same as that of the corresponding Q CF due to CF mechanism. The relative importance of CT mechanism (characterized by Q CT/ Q CF) increases with the increasing atomic number of ligand X. So, for 3d n ion clusters in crystals with heavy element ligand ion (e.g., Br −), the reasonable explanations of SH parameters should contain the contributions from both CF and CT mechanisms.

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