<p>The regression equation correlating the doping concentration of Er<sup>3+</sup>/Yb<sup>3+</sup> with luminescence intensity was established from a theoretical model, which was further refined through experimental optimization design. Then, the optimal solution of the equation was calculated by genetic algorithm, and the doping concentrations of Er<sup>3+</sup> and Yb<sup>3+</sup> were obtained to be 5.61&#xa0;mol% and 33.55&#xa0;mol% under 980&#xa0;nm near-infrared radiation excitation, and 5.58&#xa0;mol% and 28.88&#xa0;mol% under 1550&#xa0;nm near-infrared radiation excitation, respectively. Then, the Er<sup>3+</sup>/Yb<sup>3+</sup> co-doped BaGeTeO<sub>6</sub> up-conversion phosphors powder was synthesized by high-temperature solid phase method. And the crystal structure of the resulting fluorescent powder was analysed by X-ray diffraction to confirm that the optimal BaGeTeO<sub>6</sub> samples were pure phase. The up-conversion fluorescence emission spectra of the samples were measured under 980&#xa0;nm and 1550&#xa0;nm pumping conditions, and strong green and red emissions were found with peaks at around 532&#xa0;nm, 555&#xa0;nm and 672&#xa0;nm, corresponding to the jumps of the <sup>2</sup>H<sub>11/2</sub>→<sup>4</sup>I<sub>15/2</sub>, <sup>4</sup>S<sub>3/2</sub>→<sup>4</sup>I<sub>15/2</sub> and <sup>4</sup>F<sub>9/2</sub>→<sup>4</sup>I<sub>15/2</sub> energy levels, respectively. For the optimal samples under these two pumping conditions, the relationship between the up-converted fluorescence and the laser operating current is explored.The up-converted fluorescence in these two cases is shown to be a two-photon and three-photon process, respectively, and the mechanism of the up-converted fluorescence is analysed and discussed in detail. In addition, the relationship between the up-conversion fluorescence and the temperature of the optimal samples is also investigated, revealing the excellent temperature sensing properties of the up-conversion emission under 980&#xa0;nm and 1550&#xa0;nm near-infrared radiation excitation.</p>

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Experimental optimization design for up-conversion luminescence properties and FIR based optical temperature sensing in BaGeTeO6: Er3+, Yb3+ fluorescent materials

  • Shengyi Liu,
  • Duan Gao,
  • Xin Chen,
  • Li Wang,
  • Wenbin Song,
  • Han Yin,
  • Ying Zhu,
  • Shang Gao,
  • Jingjing Zhang

摘要

The regression equation correlating the doping concentration of Er3+/Yb3+ with luminescence intensity was established from a theoretical model, which was further refined through experimental optimization design. Then, the optimal solution of the equation was calculated by genetic algorithm, and the doping concentrations of Er3+ and Yb3+ were obtained to be 5.61 mol% and 33.55 mol% under 980 nm near-infrared radiation excitation, and 5.58 mol% and 28.88 mol% under 1550 nm near-infrared radiation excitation, respectively. Then, the Er3+/Yb3+ co-doped BaGeTeO6 up-conversion phosphors powder was synthesized by high-temperature solid phase method. And the crystal structure of the resulting fluorescent powder was analysed by X-ray diffraction to confirm that the optimal BaGeTeO6 samples were pure phase. The up-conversion fluorescence emission spectra of the samples were measured under 980 nm and 1550 nm pumping conditions, and strong green and red emissions were found with peaks at around 532 nm, 555 nm and 672 nm, corresponding to the jumps of the 2H11/24I15/2, 4S3/24I15/2 and 4F9/24I15/2 energy levels, respectively. For the optimal samples under these two pumping conditions, the relationship between the up-converted fluorescence and the laser operating current is explored.The up-converted fluorescence in these two cases is shown to be a two-photon and three-photon process, respectively, and the mechanism of the up-converted fluorescence is analysed and discussed in detail. In addition, the relationship between the up-conversion fluorescence and the temperature of the optimal samples is also investigated, revealing the excellent temperature sensing properties of the up-conversion emission under 980 nm and 1550 nm near-infrared radiation excitation.