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Investigation of the optical spectra and spin-Hamiltonian parameters for the rhombic \(\mathrm{Cu}^{2+}\) center in \(\beta\mathrm{-Ca}_3(\mathrm{PO}_4)_2\). (English) Zbl 1264.82147

Summary: The four optical band positions and six spin-Hamiltonian parameters (the \(g\) factors \(g_i\) and the hyperfine structure constants \(A_i,\;i = x, y, z\)) for the rhombic \(\mathrm{Cu}^{2+}\)-center in \(\beta\mathrm{-Ca}_3(\mathrm{PO}_4)_2\) are calculated by two theoretical methods, namely the complete diagonalization (of energy matrix) method and the perturbation theory method (PTM). Both methods are based on the cluster approach, in which the covalence due to admixture of ligands to the central metal ion is considered. The calculated results of the two methods are close to each other and agree with the experimental values. This suggests that both methods are effective in explaining the optical and electron paramagnetic resonance data for \(d^9\) ions in crystals. The calculations also show that although the admixture of \(|d^2_z\rangle\) to the ground state wave function is small, it should not be neglected in calculations of spin-Hamiltonian parameters. So, in PTM, the high-order perturbation formulae of spin-Hamiltonian parameters based on the cluster approach for \(d^9\) ion in rhombic symmetry should be derived by taking into account the admixture of the \(|d^2_z\rangle\) state to the \(|d_{x^{2}-y^{2}}\rangle\) ground state.

MSC:

82D25 Statistical mechanics of crystals
81Q10 Selfadjoint operator theory in quantum theory, including spectral analysis

Keywords:

optical spectra
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