An electron paramagnetic resonance (EPR) study of a synthetic single crystal of LiScGeO• doped with Cr ions earried out earlier at the X-and Q-bands at 300 K has indicated additional weak lines. A detailed analysis of these EPR lines, which were tentatively attributed to the Fe 3+ ions at two different mirror symmetry sites, is presented in this paper. The angular dependences in the three crystallographic planes were resolved by fitting the two distinct spectra denoted Fe3+(l) and Fe3+(II) with a spin Hamiltonian (S = 5/2) of monoclinic symmetry. The rank-4 crystal field tensors at tetrahedral and octahedral sites were calculated with the point-charge model to determine the principal axis ofientations of their cubic, letragonal and trigonal components. A comparative analysis of the zero-field splitting tensors and the crystal field ones indicates that Fe3+(I) ions substitute for Sc 3 § at octahedral sites and Fe3+(II) ions substitute for Ge 4~ at tetrahedral sites with no significant distortion of the coordination polyhedra in the structure of LiScGeO 4.
IntroduetionThe structure of LiScGeO 4 belongs to the orthorhombic space group D~ 6 Pnma with a = 1.0673 nm, b = 0.59926 nm, c = 0.49667 nm [1]. Fe 3+ ions in low concentrations ate usual traces in the natural and synthetic crystals with olivine type structure thus determining their spectroscopic properties. In forsterite Mg2SiO a, Fe 3+ ions were established as substituting at all the three structurally nonequivalent cationic sites [2, 3]: the octahedral MI (4a) and M2 (4c) sites, and the tetrahedral (4c) sites. In chrysoberyl A12BeO 4, Fe 3+ ions were established as substituting for Al 3+ at the octahedral M2 site [4]. Previously we have reported [5] that in the Cr-doped crystal of LiScGeO 4, along with electron paramagnetic reso-