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The ESR spectra of Mn2+ ions have been observed in borate glasses of the composition (MnO)x(B2O3+0.04 K2O)1−x with x from 0.001 up to 0.030. For small concentrations of Mn2+ the central fine-structure transitions (M = +½↔—½), although broadened by the random orientation of small noncubic crystalline fields, show a well-resolved hyperfine structure. In addition to the Δm=0 transitions, ``forbidden'' Δm=±1 have been observed. The spectra prove that the coordination of the O2− ions around the Mn2+ ions is mainly cubic, but that small deformations of the cubic symmetry exist. The deformations vary from ion to ion, and range up to average values of the order of 5% in the interionic distances and 10 deg in the angles. The discussion has been based on a spin Hamiltonian involving an isotropic g factor, fine structure term D, and hyperfine structure term A. The line positions have been calculated up to the third order in D and A. The numerical results are: g=2.002±0.002, | A | /hc= (87–2)×10−4 cm−1, and DAv/hc= (89±10)×10−4 cm−1, the latter value representing an average over all deviations from cubic symmetry.
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Wijn et al. (1967) studied this question.
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