In comparison to other chalcogenide glasses, Ge-Ga-S glasses have the largest rare-earth solubility. Raman spectra of GeS_(2)-Ga_(2)S_(3) glasses contain two bands at 265 and 385 cm^(-1) which increased in intensity with the addition of Ga_(2)S_(3). ...
In comparison to other chalcogenide glasses, Ge-Ga-S glasses have the largest rare-earth solubility. Raman spectra of GeS_(2)-Ga_(2)S_(3) glasses contain two bands at 265 and 385 cm^(-1) which increased in intensity with the addition of Ga_(2)S_(3). These are associated with the vibration of Ge-Ge bonds and edge-shared GaS_(4) tetrahedra, respectively. Upon the addition of La_(2)S_(3) into GeS_(2)-Ga_(2)S_(3) glasses, intensities of these two bands decreased while a new band appeared at 375 cm^(-1) due to the vibration of tetrahedra with non-bridging sulfur(s). Dissociation of Ge-Ge bonds and edge-shared GaS_(4) tetrahedra through the addition of La_(2)S_(3) are responsible for the non-bridging sulfur formation. La^(3+) can be dissolved into the glass network as charge compensators for these non-bridging sulfurs. Since no such structural unit is present in glasses without Ga_(2)S_(3), this connection scheme and the structural modification in Ga-containing chalcogenide glasses seem to be crucial for an increase of La^(3+) solubility.