Abstract

The electron paramagnetic resonance (EPR) parameters ($g$ factors $g_{i}$ and the hyperfine structure constants ${{A}}_{{i}}$, ${i} = {x}, {y}, {z}$) are interpreted by using the perturbation formulae for a $3{d}^{9}$ ion in rhombically ({D}$_{2h}$) elongated octahedra. In the calculated formulae, the crystal field parameters are set up from the superposition model, and the contribution to the EPR parameters from the admixture of $d$-orbitals in the ground state wave function of the Cu$^{2+}$ ion was taken into account. Based on the calculation, local structural parameters of the impurity Cu$^{2+}$ center in Cd$_{2}$(NH$_{4}$)$_{2}$(SO$_{4}$)$_{3}$ (CAS) crystal were obtained (i.e., ${R}_{{x}}\approx 2.05$ {\AA}, ${R}_{{y}} \approx 1.91$ {\AA}, ${R}_{{z}} \approx 2.32$ {\AA}). The theoretical EPR parameters based on the above Cu$^{2+}$-O$^{2-}$ bond lengths in CAS crystal show a good agreement with the observed values. The results are discussed.

Highlights

  • Single crystal Cd2(NH4)2(SO4)3 (CAS) has attracted interest of researchers due to the unique dielectric [1], phase transition [2], optical [3], birefringent and electrooptical properties [4]

  • The Electron paramagnetic resonance (EPR) method provides a detailed description of the ground state of paramagnetic ions and enables one to explain the nature of crystal field and its symmetry produced by ligands around the metal ion [5,6,7]

  • Considering that (i) the data on local structures and electronic states for Cu2+ in the CAS single crystal would be helpful in understanding the microscopic mechanisms of EPR behaviors of this material containing Cu2+ dopants and (ii) the anisotropic g factors for a d 9 ion in crystals are sensitive to its immediate environment

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Summary

Introduction

Single crystal Cd2(NH4)2(SO4) (CAS) has attracted interest of researchers due to the unique dielectric [1], phase transition [2], optical [3], birefringent and electrooptical properties [4]. The EPR method provides a detailed description of the ground state of paramagnetic ions and enables one to explain the nature of crystal field and its symmetry produced by ligands around the metal ion [5,6,7] Among these transition metal ions, Cu2+ ions with 3d 9 configuration are widely used as paramagnetic probes as they represent a relatively simple one-hole magnetic system which can be used to obtain information regarding the electron wave function when there is a ligand field of low symmetry. Considering that (i) the data on local structures and electronic states for Cu2+ in the CAS single crystal would be helpful in understanding the microscopic mechanisms of EPR behaviors of this material containing Cu2+ dopants and (ii) the anisotropic g factors for a d 9 ion in crystals are sensitive to its immediate environment (and to defect structure of d 9 impurity center). The Cu2+–O2− bond lengths are obtained as follows: Rx ≈ 2.05 Å, Ry ≈ 1.91 Å, Rz ≈ 2.32 Å

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