• Photonics Research
  • Vol. 9, Issue 10, 2037 (2021)
Jing Liu1、5、*, Flavia Artizzu2、3、6、*, Min Zeng2, Luca Pilia4, Pieter Geiregat2, and Rik Van Deun2
Author Affiliations
  • 1Key Laboratory of Luminescence Analysis and Molecular Sensing, Ministry of Education, School of Materials and Energy, Southwest University, Chongqing 400715, China
  • 2Department of Chemistry, Ghent University, B-9000 Ghent, Belgium
  • 3Department of Sciences and Technological Innovation, University of Eastern Piedmont “Amedeo Avogadro”, 15121 Alessandria, Italy
  • 4Department of Mechanical, Chemical and Material Engineering, University of Cagliari, 09123 Cagliari, Italy
  • 5e-mail: jingliu77@swu.edu.cn
  • 6e-mail: flavia.artizzu@ugent.be
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    DOI: 10.1364/PRJ.433192 Cite this Article Set citation alerts
    Jing Liu, Flavia Artizzu, Min Zeng, Luca Pilia, Pieter Geiregat, Rik Van Deun. Dye-sensitized Er3+-doped CaF2 nanoparticles for enhanced near-infrared emission at 1.5 μm[J]. Photonics Research, 2021, 9(10): 2037 Copy Citation Text show less
    Mechanism of ET in FITC sensitized Er3+-doped CaF2 nanoparticles.
    Fig. 1. Mechanism of ET in FITC sensitized Er3+-doped CaF2 nanoparticles.
    (a) TEM image and (b) powder XRD pattern of CaF2:Er3+ nanoparticles.
    Fig. 2. (a) TEM image and (b) powder XRD pattern of CaF2:Er3+ nanoparticles.
    (a) Absorption spectra; (b) Vis emission spectra (λex=467 nm); and (c) luminescence decay curves (λex=467 nm; λem=538 nm) of FITC (black), CaF2@FITC (blue), CaF2:Er3+@FITC (red). Steady-state spectra are normalized for the absorbed power at excitation wavelength.
    Fig. 3. (a) Absorption spectra; (b) Vis emission spectra (λex=467  nm); and (c) luminescence decay curves (λex=467  nm; λem=538  nm) of FITC (black), CaF2@FITC (blue), CaF2:Er3+@FITC (red). Steady-state spectra are normalized for the absorbed power at excitation wavelength.
    (a) Optimized geometries and (b) MOs calculated by DFT methods at B3LYP/6-311 + G(d,p) level of theory (color codes: Ca, green; C, gray; O, red; N, purple; S, yellow; H, white). The orbitals are reported with a contour value of 0.050.
    Fig. 4. (a) Optimized geometries and (b) MOs calculated by DFT methods at B3LYP/6-311 + G(d,p) level of theory (color codes: Ca, green; C, gray; O, red; N, purple; S, yellow; H, white). The orbitals are reported with a contour value of 0.050.
    (a) NIR emission spectra of CaF2:Er3+ (black, λex=378 nm corresponding to the Er3+4G11/2←4I15/2 transition) and CaF2:Er3+@FITC (red, λex=467 nm corresponding to the maximum of the FITC dye absorption); (b) luminescence decay curves of CaF2:Er3+ (black, λex=378 nm; λem=1530 nm) and CaF2:Er3+@FITC (red, λex=467 nm; λem=1530 nm). Steady-state spectra are normalized for the absorbed power at excitation wavelength.
    Fig. 5. (a) NIR emission spectra of CaF2:Er3+ (black, λex=378  nm corresponding to the Er3+4G11/24I15/2 transition) and CaF2:Er3+@FITC (red, λex=467  nm corresponding to the maximum of the FITC dye absorption); (b) luminescence decay curves of CaF2:Er3+ (black, λex=378  nm; λem=1530  nm) and CaF2:Er3+@FITC (red, λex=467  nm; λem=1530  nm). Steady-state spectra are normalized for the absorbed power at excitation wavelength.
    Two-dimensional (2D) TA (ΔA) map of (a) FITC; (b) CaF2@FITC; and (c) CaF2:Er3+@FITC in chloroform as a function of wavelength and time, upon photoexcitation at 500 nm; (d) representative selection of TA spectra of CaF2:Er3+@FITC in chloroform at different time delays, the black and gray dashed lines show the inverted PL spectrum and ground-state absorption spectrum, respectively; (e) selection of TA spectra of FITC, CaF2@FITC, and CaF2:Er3+@FITC in chloroform at 7.5 ps time delay; (f) selected kinetics of FITC, CaF2@FITC, and CaF2:Er3+@FITC for the SE signal at 550 nm in the sub-nanosecond time range.
    Fig. 6. Two-dimensional (2D) TA (ΔA) map of (a) FITC; (b) CaF2@FITC; and (c) CaF2:Er3+@FITC in chloroform as a function of wavelength and time, upon photoexcitation at 500 nm; (d) representative selection of TA spectra of CaF2:Er3+@FITC in chloroform at different time delays, the black and gray dashed lines show the inverted PL spectrum and ground-state absorption spectrum, respectively; (e) selection of TA spectra of FITC, CaF2@FITC, and CaF2:Er3+@FITC in chloroform at 7.5 ps time delay; (f) selected kinetics of FITC, CaF2@FITC, and CaF2:Er3+@FITC for the SE signal at 550 nm in the sub-nanosecond time range.
    (a) Spectral overlap of Er3+ absorption cross section (red) and FITC fluorescence spectrum normalized to unity (black curve with shaded area). (b) FITC to Er3+ sensitization efficiency (ηsens) calculated by the Förster’s model as a function of the donor–acceptor distance (R). Inset, DFT-calculated optimized geometry for FITC coordinated to Ca2+ where the light blue arrow represents the TD-DFT calculated S1−S0 transition dipole moment.
    Fig. 7. (a) Spectral overlap of Er3+ absorption cross section (red) and FITC fluorescence spectrum normalized to unity (black curve with shaded area). (b) FITC to Er3+ sensitization efficiency (ηsens) calculated by the Förster’s model as a function of the donor–acceptor distance (R). Inset, DFT-calculated optimized geometry for FITC coordinated to Ca2+ where the light blue arrow represents the TD-DFT calculated S1S0 transition dipole moment.
    Sampleτ (ps)ηsens (%)
    FITC
    CaF2200 (10)
    Er3+15 (2)92
    Table 1. FITC-Excited Singlet Ultrafast Decay Time Constants and FITC to Er3+ Sensitization Efficiency Calculated through Eq. (1)
    Jing Liu, Flavia Artizzu, Min Zeng, Luca Pilia, Pieter Geiregat, Rik Van Deun. Dye-sensitized Er3+-doped CaF2 nanoparticles for enhanced near-infrared emission at 1.5 μm[J]. Photonics Research, 2021, 9(10): 2037
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