Glasses were prepared using a melt-quenching technique with the following composition: 55 mol% Li2B4O7 and (45-x) mol% Pb3O4- (x) mol% CuO, where x takes values of 5, 10, 15, 20 and 25 mol%. Differential thermal analysis (DTA) confirmed the formation of glass, revealing that the glass transition temperature increased from 300 °C to 317 °C as the copper content rose to 20 mol%. However, beyond this point, the glass transition temperature began to decrease. Some samples displayed two glassy phases, as indicated by the presence of two distinct glass transition temperatures. All glass samples demonstrated high thermal stability and effective glass-forming ability, with properties improving as the copper content increased. X-ray diffraction (XRD) spectra confirmed that the samples were amorphous in nature. The structural, optical, and luminescence properties were investigated using Fourier-transform attenuated total reflectance (ATR) FTIR, X-ray photoelectron spectroscopy (XPS), UV/Vis/NIR spectroscopy, and a spectrofluorometer. FTIR spectra indicated that the glass samples contained vibrations from BO4, BO3, and PbO4 groups. As the amount of copper oxide increased, the concentration of non-bridging oxygens (NBOs) also rose. The ratio of BO4 to BO3 increased up to 20 mol% of CuO and subsequently began to decrease. According to the XPS results, the ratio of NBOs to bridging oxygens (BOs) increased with CuO content up to 15 mol%, after which it declined. This initial rise suggests an increase in polarization and a loosening of the glass network structure. Additionally, copper ions were present in both Cu2+ and Cu+ valence states, in line with the optical absorption results. The ratio of Cu²⁺ to Cu⁺ increases to 6 as the concentration of copper rises. As the copper oxide content increased, the optical band gap decreased from 2.9 eV to 1.7 eV. Luminescence from copper ions produced emissions in various colors, including green, greenish-yellow, orange, and pink, depending on the excitation wavelengths, which ranged from 270 nm to 350 nm without a filter. Using a filter, the emissions took on a blue hue at the same excitation energy.
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