High purity (GeS 2) 80− x (Ga 2S 3) 20· xNdCl 3 ( x=1, 2, 3) and (GeS 2) 79(Ga 2S 3) 20·Nd 2O 3 glasses were prepared and their thermal and optical properties measured. The GeS 2–Ga 2S 3 glasses can dissolve relatively large amounts of NdCl 3 and Nd 2O 3 (≤3 mol%) and still form stable glasses. They are optically transparent in the range from 19000 cm −1 to 800 cm −1. The glass transition temperature ( T g≅378°C) and the glass-forming criteria are only slightly changed by Nd doping (Δ T=147°C, H r=0.78; H′=0.39, S=4.10 K, where Δ T= T c− T g, H r is Hruby's criterion, H r=( T c− T g)/( T m− T c), H′=( T c− T g)/ T g, and S=( T c− T x)( T c− T g)/ T g). The short-wavelength absorption edge lies near 2.7 eV, doping with Nd creates new absorption bands which can be assigned to electron transfer from the 4 I 9/2 level to 4 G 7/2, 4 G 9/2, 2 K 13/2, 2 G 5/2, 2 G 7/2, 2 H 11/2, 4 F 9/2, 4 F 7/2, 4 S 3/2, 2 H 9/2, 4 F 5/2, 4 F 3/2, 4 I 15/2, 4 I 13/2 and 4 I 11/2 levels. In doped glasses, several broad luminescence bands, near 910, 1080 and 1360 nm, were found, which can be assigned to the transitions from 4 F 3/2 to 4 I 9/2, to 4 I 11/2 and to 4 I 13/2 electron levels. The long-wavelength absorption edge was found near 1000 cm −1 and is due to multiphonon Ge–S and Ga–S vibrations.
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