<p>Green fluorescence emitting TeO<sub>2</sub> + WO<sub>3</sub> + GeO<sub>2</sub> + Ho<sub>2</sub>O<sub>3</sub> glasses containing different Ho<sup>3+</sup> doping (TWGHo<i>x</i>) were prepared by melt quench technique. The glassy phase was examined through powder X-ray diffraction. Several spectroscopic properties were calculated from optical absorption spectral results adopting Judd–Ofelt theory. The pumping wavelength producing efficient fluorescence was selected as 454&#xa0;nm. The Ho<sup>3+</sup> doping was optimized as 0.5&#xa0;mol% based on concentration-dependent emission study. Upon 454&#xa0;nm pumping, TWGHo<i>x</i> reveals two fluorescence bands positioned at 548&#xa0;nm and 660&#xa0;nm due to (<sup>5</sup>S<sub>2</sub> + <sup>5</sup>F<sub>4</sub>) → <sup>5</sup>I<sub>8</sub> and <sup>5</sup>F<sub>5</sub> → <sup>5</sup>I<sub>8</sub> transitions, respectively. Thermal sensitivity was examined through temperature dependence fluorescence study. The effect of Ho<sup>3+</sup> doping on emitted color and its purity was studied. Fluorescence decay dynamics of (<sup>5</sup>S<sub>2</sub> + <sup>5</sup>F<sub>4</sub>) levels were studied controlling <i>λ</i><sub>ex</sub> = 454&#xa0;nm and <i>λ</i><sub>em</sub> = 548&#xa0;nm. The fluorescence quantum efficiency was calculated from the decay time, while the fluorescence quantum yield was estimated using an integrating sphere connected to a spectrofluorimeter. The quenching in luminescence and decay time were ascribed to non-radiative cross-relaxation transitions. The applicability for green laser source was verified by calculating emission cross-sections, gain band width, figure of merit, quantum efficiency, and quantum yield.</p>

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Green fluorescent Ho3+-doped TeO2 + WO3 + GeO2 + Ho2O3 glasses for lighting devices

  • B. C. Jamalaiah,
  • K. Venkata Rao,
  • G. Pullaiah

摘要

Green fluorescence emitting TeO2 + WO3 + GeO2 + Ho2O3 glasses containing different Ho3+ doping (TWGHox) were prepared by melt quench technique. The glassy phase was examined through powder X-ray diffraction. Several spectroscopic properties were calculated from optical absorption spectral results adopting Judd–Ofelt theory. The pumping wavelength producing efficient fluorescence was selected as 454 nm. The Ho3+ doping was optimized as 0.5 mol% based on concentration-dependent emission study. Upon 454 nm pumping, TWGHox reveals two fluorescence bands positioned at 548 nm and 660 nm due to (5S2 + 5F4) → 5I8 and 5F5 → 5I8 transitions, respectively. Thermal sensitivity was examined through temperature dependence fluorescence study. The effect of Ho3+ doping on emitted color and its purity was studied. Fluorescence decay dynamics of (5S2 + 5F4) levels were studied controlling λex = 454 nm and λem = 548 nm. The fluorescence quantum efficiency was calculated from the decay time, while the fluorescence quantum yield was estimated using an integrating sphere connected to a spectrofluorimeter. The quenching in luminescence and decay time were ascribed to non-radiative cross-relaxation transitions. The applicability for green laser source was verified by calculating emission cross-sections, gain band width, figure of merit, quantum efficiency, and quantum yield.