• Chinese Optics Letters
  • Vol. 15, Issue 5, 051604 (2017)
Fangwei Qi1, Feifei Huang1、*, Tao Wang1, Ruoshan Lei1, Junjie Zhang1, Shiqing Xu1, and Long Zhang1、2
Author Affiliations
  • 1College of Materials Science and Engineering, China Jiliang University, Hangzhou 310018, China
  • 2Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
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    DOI: 10.3788/COL201715.051604 Cite this Article Set citation alerts
    Fangwei Qi, Feifei Huang, Tao Wang, Ruoshan Lei, Junjie Zhang, Shiqing Xu, Long Zhang. Influence of Tm3+ ions on the amplification of Ho3+:5I75I8 transition in fluoride glass modified by Al(PO3)3 for applications in mid-infrared optics[J]. Chinese Optics Letters, 2017, 15(5): 051604 Copy Citation Text show less
    DSC curve of the AYF glass with 5 mol% Al(PO3)3 introduction. Raman spectrum in the 100–1200 cm−1 range of undoped RE ions AYF glass with Al(PO3)3 introduction.
    Fig. 1. DSC curve of the AYF glass with 5 mol% Al(PO3)3 introduction. Raman spectrum in the 1001200cm1 range of undoped RE ions AYF glass with Al(PO3)3 introduction.
    Absorption spectra of Tm3+ and Ho3+ singly doped and codoped samples. The inset is the transmittance spectrum of the sample.
    Fig. 2. Absorption spectra of Tm3+ and Ho3+ singly doped and codoped samples. The inset is the transmittance spectrum of the sample.
    Fluorescence spectra of Tm3+/Ho3+ codoped AYF glass modified by Al(PO3)3 with (a) different Ho3+ concentrations and (b) different Tm3+ concentrations. (c) The inset shows the energy level scheme of the Tm3+/Ho3+ system. ETU, ET upconversion.
    Fig. 3. Fluorescence spectra of Tm3+/Ho3+ codoped AYF glass modified by Al(PO3)3 with (a) different Ho3+ concentrations and (b) different Tm3+ concentrations. (c) The inset shows the energy level scheme of the Tm3+/Ho3+ system. ETU, ET upconversion.
    (a) decay curves of Ho3+ in the HT1-4 samples, where the Ho3+ concentration is fixed at 0.2 mol% and (b) ET efficiencies from Tm3+ to Ho3+ in the TH1-4 samples.
    Fig. 4. (a) decay curves of Ho3+ in the HT1-4 samples, where the Ho3+ concentration is fixed at 0.2 mol% and (b) ET efficiencies from Tm3+ to Ho3+ in the TH1-4 samples.
    Absorption cross section and emission cross section of the Ho3+:I85→I75 transition in the HT4 sample at the 2.0 μm region. The inset shows the products of the emission cross section and measured decay lifetime (σemi×τ) in the HT1-4 samples.
    Fig. 5. Absorption cross section and emission cross section of the Ho3+:I85I75 transition in the HT4 sample at the 2.0 μm region. The inset shows the products of the emission cross section and measured decay lifetime (σemi×τ) in the HT1-4 samples.
    Ωλ(×1020cm2)Ω2Ω4Ω6Ω4/Ω6Reference
    Fluoride1.861.901.321.43[29]
    Phosphate5.602.721.871.45[29]
    Silicate5.842.381.751.36[30]
    AYF-Al(PO3)32.22±0.023.85±0.041.88±0.022.04Present
    δrms0.18×106
    Table 1. J-O Parameters Ωλ of Ho3+ in Various Glasses
    Transitionλ (nm)A(s1)ΣA(s1)βτ (ms)
    I75I851944118.74118.74±0.1100.00%±0.2%8.42
    I65I851152215.09254.4684.53%3.93
    I75281039.3715.47%
    I55I8588781.16204.1239.76%4.90
    I751631107.7352.78%
    I65389015.237.46%
    I45I8575710.95111.269.84%8.99
    Table 2. Predicted Spontaneous Transition Probability (A), Total Spontaneous Transition Probability (ΣA), Branching Ratios (β), and Radiative Lifetimes (τrad) of AYF Glass Modified by Al(PO3)3 for Various Selected Excited Levels of Ho3+
    IonsGlassσemi(1021cm2)Reference
    Tm3+/Ho3+AYF-Al(PO3)37.60Present work
    Fluorophosphate6.15[31]
    Silicate3.07[37]
    Yb3+/Ho3+Fluorophosphate4.53[20]
    Silicate5.05[38]
    Yb3+/Tm3+/Ho3+Phosphate4.21[39]
    Fluorophosphate5.50[40]
    Table 3. σemi of 2.0 μm of Ho3+ in Various RE-Ion-Doped Glasses
    Fangwei Qi, Feifei Huang, Tao Wang, Ruoshan Lei, Junjie Zhang, Shiqing Xu, Long Zhang. Influence of Tm3+ ions on the amplification of Ho3+:5I75I8 transition in fluoride glass modified by Al(PO3)3 for applications in mid-infrared optics[J]. Chinese Optics Letters, 2017, 15(5): 051604
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