Glass systems of composition (100− x) Na 2B 4O 7·10H 2O+ x MnSO 4·H 2O ( x = 0 , 0.1, 0.3, 0.5, 0.75, 1, 1.25, 1.5, 1.75 and 2 mol%) have been studied by using electron paramagnetic resonance (EPR) and optical absorption techniques. The room temperature EPR spectra exhibit resonance signals at g ≈ 2.0 with a sextet hyperfine structure (hfs) besides two weak signals at g ≈ 3.3 and 4.3. The resonance signal at g ≅ 2.0 is due to Mn 2+ ions in an environment close to octahedral symmetry, whereas the resonances at g ≅ 3.3 and 4.3 are attributed to the rhombic surroundings of the Mn 2+ ions. It is observed that for x = 1.25 mol % in sodium tetra borate glasses (NTB) the EPR spectrum exhibits a good resolution of allowed as well as forbidden hfs at g ≈ 2.0 . The Mn 2+ ions in NTB glasses (with A ≈ 95 G ) are quite ionic in nature. The number of spins ( N) participating in resonance at g ≈ 2.0 has been calculated by comparing the area under the absorption curve with that of a standard of known concentration. A linear relationship is observed between log N and 1/ T in accordance with the Boltzmann law. Magnetic susceptibilities ( χ ) were calculated from the EPR spectra at different temperatures. The susceptibility is varying inversely with temperature in accordance with the Curie law, and the Curie constant is evaluated from the 1 / χ versus T graph. The zero-field splitting parameter D has also been calculated from the allowed hyperfine (HF) lines. The D value was found to be dependent on temperature. The optical absorption spectrum exhibits a single broad band centered around 470 nm and was assigned to the 6A lg(S)→ 4T lg(G) transition. From the ultra violet absorption edges the optical bandgap and Urbach energies have been evaluated.
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