Abstract

The zero-field splitting of ${\mathrm{S}}^{6}$-state ions is studied in the intermediate-field coupling scheme by taking the crystal-field and the electrostatic interactions as the unperturbed Hamiltonian and the spin-orbit interaction as a perturbation. This perturbation process shows a very good convergence and provides a comprehensive approach to the derivation of both the rank-2 ${\mathrm{b}}_{2}^{\mathrm{q}}$ and the rank-4 ${\mathrm{b}}_{4}^{\mathrm{q}}$ zero-field splitting parameters, which are shown to come predominantly from the first nonzero peturbation terms. Cubic and tetragonal symmetries are considered and the zero-field splitting parameters D (\ensuremath{\sim}${\mathrm{b}}_{2}^{0}$), a (\ensuremath{\sim}${\mathrm{b}}_{4}^{4}$), and F (\ensuremath{\sim}${\mathrm{b}}_{4}^{0}$) are investigated in detail as functions of the cubic Dq and the tetragonal crystal-field (CF) parameters ${\mathrm{B}}_{20}$ and ${\mathrm{B}}_{40}^{\ensuremath{'}}$. It is found that the tetragonal CF components ${\mathrm{B}}_{20}$ and ${\mathrm{B}}_{40}^{\ensuremath{'}}$ contribute, to the cubic zero-field splitting parameter a, a value ${\mathrm{a}}_{\mathrm{t}}$, which is non-negligible. The ratio ${\mathrm{a}}_{\mathrm{t}}$/F is found to be insensitive to CF parameters and to lie in the range -0.2 to -0.5. Both parameters ${\mathrm{a}}_{\mathrm{t}}$ and F depend mainly on ${\mathrm{B}}_{20}$, whereas D depends mainly on ${\mathrm{B}}_{40}^{\ensuremath{'}}$. The results of earlier perturbation procedures are also calculated and compared with the present ones. The present theory deals with the zero-field splitting parameters ${\mathrm{b}}_{4}^{\mathrm{q}}$ (k=2 and 4) by regarding the crystal-field parameters ${\mathrm{B}}_{\mathrm{kq}}$ (k=2 and 4) as freely adjustable phenomenological parameters, thus avoiding problems arising from the application of a specific crystal-model to the evaluation of ${\mathrm{B}}_{\mathrm{bq}}$. Following this idea, numerical calculations are carried out for the parameters a, D, and F for ${\mathrm{Mn}}^{2+}$ and ${\mathrm{Fe}}^{3+}$ ions in cubic and tetragonal fluoroperovskites. The results are in good agreement with experimental data. This work presents examples where the crystal-field theory allows a successful interpretation of the zero-field splitting of ${\mathrm{S}}^{6}$-state ions.

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