glass in this work is lower than that of phosphate glass. According to the investigation by Weyl, [6] the above results are on account of the multiabsorption of V 4+ and V 3+ . If one could adjust the composition and modify the procedure properly, more V 3+ and V 4+ states could be converted into the V 5+ state, and the transmission of the vanadate glass would likely be much better. In summary, a novel vanadate glass with remarkable optical transmission was fabricated for the first time. The vanadate glass used in this experiment is suitable for optical applications. Furthermore, when doped with neodymium, it demonstrated quite encouraging laser properties. The results indicated the feasibility of utilizing the novel transparent vanadate glasses in optics, especially in laser-related fiber optics.
ExperimentalThe glass samples were prepared from high purity materials. The composition of the sample materials was carefully monitored and the experimental conditions were controlled to obtain a higher concentration of V 5+ in the glass samples. After hundreds of experiments, the glass was developed from the traditional binary composition to a quaternary one: 28V 2 O 5 ±22SiO 2 ±23MO (CaO, BaO, SrO)±27X 2 O (Na 2 O, K 2 O, Cs 2 O) in weight percentage. The batch materials were melted in a platinum crucible inside a silica tube heated by a medium induction furnace. Oxygen gas of 99.99% purity was introduced into the silica tube throughout the whole melting process. The crucible was heated at 1650 K for 2 h. The melted substances were then cast in a graphite mould and annealed. All the samples were fabricated to the size of 25 mm 20 mm 5 mm and optically polished.The absorption spectra were measured using a HITACHI330 spectrometer at room temperature (295 K). The IR spectra were measured using a SHIMADZU RF±5301PC at room temperature. The emission spectra were obtained by exciting the samples with an 805 nm diode laser. The light from the light source was chopped at 80 Hz and focused onto the 5 mm 25 mm faces of the samples. One millimeter from the edge was excited to minimize the re-absorption of the emission. The emission from the samples was focused to a monochrometer and detected by a germanium detector. The signal was intensified with a lock-in amplifier and processed by a computer.The fluorescence lifetime was measured by exciting the samples with a xenon lamp and detected by an S-1 photomultiplier tube. The fluorescence decay curves were recorded and averaged by a computer-controlled transient digitizer. The stimulated-emission cross-section of the neodymium-doped vanadate glass was calculated according to the Judd±Ofelt theory [9,10].