• Spectroscopy and Spectral Analysis
  • Vol. 41, Issue 1, 71 (2021)
Chang-qing YE*, Xue YU, Shuo-ran CHEN, Zuo-qin LIANG, Yu-yang ZHOU, and Xiao-mei WANG
Author Affiliations
  • Research Center for Green Printing Nanophotonic Materials, School of Materials Science and Engineering, Suzhou University of Science and Technology, Suzhou 215009, China
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    DOI: 10.3964/j.issn.1000-0593(2021)01-0071-09 Cite this Article
    Chang-qing YE, Xue YU, Shuo-ran CHEN, Zuo-qin LIANG, Yu-yang ZHOU, Xiao-mei WANG. Study on the Structure/Energy-Level of Palladuim-Porphyrin Sensitizers on the Triplet-Triplet-Annihilation Upconversion Performance[J]. Spectroscopy and Spectral Analysis, 2021, 41(1): 71 Copy Citation Text show less
    The synthetic procedure of OEP
    Fig. 1. The synthetic procedure of OEP
    The synthetic procedure of PdOEP
    Fig. 2. The synthetic procedure of PdOEP
    The synthetic procedure of BrTPP
    Fig. 3. The synthetic procedure of BrTPP
    The synthetic procedure of PdBrTPP
    Fig. 4. The synthetic procedure of PdBrTPP
    The synthetic procedure of p-DHMPA
    Fig. 5. The synthetic procedure of p-DHMPA
    Optical characterization of PdOEP in n-propanol(a): Absorption spectrum; (b): Fluorescence spectrum; (c): The phosphorescence spectrum in N2 atmosphere; (excitation wavelength: 532 nm); (d): The phosphorescence decay curves associated with dual exponential fitting for PdOEP at room temperature in N2 atmosphere (Emission wavelength 665 nm)
    Fig. 6. Optical characterization of PdOEP in n-propanol
    (a): Absorption spectrum; (b): Fluorescence spectrum; (c): The phosphorescence spectrum in N2 atmosphere; (excitation wavelength: 532 nm); (d): The phosphorescence decay curves associated with dual exponential fitting for PdOEP at room temperature in N2 atmosphere (Emission wavelength 665 nm)
    Optical characterization of PdBrTPP in n-propanol(a): Absorption spectrum; (b): Fluorescence spectrum; (c): The phosphorescence spectrum in N2 atmosphere; (excitation wavelength: 532 nm); (d): The phosphorescence decay curves associated with dual exponential fitting for PdBrTPP at room temperature in N2 atmosphere (Emission wavelength 694 nm)
    Fig. 7. Optical characterization of PdBrTPP in n-propanol
    (a): Absorption spectrum; (b): Fluorescence spectrum; (c): The phosphorescence spectrum in N2 atmosphere; (excitation wavelength: 532 nm); (d): The phosphorescence decay curves associated with dual exponential fitting for PdBrTPP at room temperature in N2 atmosphere (Emission wavelength 694 nm)
    Absorption and fluorescence spectra of p-DHMPA in n-propanol solution
    Fig. 8. Absorption and fluorescence spectra of p-DHMPA in n-propanol solution
    Jablonski diagram of the TTA-UC process between the sensitizers (PdOEP, PdBrTPP) and the emitter (p-DHMPA)
    Fig. 9. Jablonski diagram of the TTA-UC process between the sensitizers (PdOEP, PdBrTPP) and the emitter (p-DHMPA)
    Concentration-dependent upconversion spectra of emitter (p-DHMPA) doped with sensitizer (a)PdOEP, (b)PdBrTPP, (c)Stern-Volmer plots of sensitizers (PdOEP and PdBrTPP) quenched by emitter p-DHMPA
    Fig. 10. Concentration-dependent upconversion spectra of emitter (p-DHMPA) doped with sensitizer (a)PdOEP, (b)PdBrTPP, (c)Stern-Volmer plots of sensitizers (PdOEP and PdBrTPP) quenched by emitter p-DHMPA
    The power-dependent upconversion spectra(a): PdOEP/p-DHMPA; (b): PdBrTPP/p-DHMPA; Inset: Logarithmic plots of the integral of upconversion peak versus power density
    Fig. 11. The power-dependent upconversion spectra
    (a): PdOEP/p-DHMPA; (b): PdBrTPP/p-DHMPA; Inset: Logarithmic plots of the integral of upconversion peak versus power density
    Under excitation of 532 nm laser (400 mW·cm-2), the concentration-dependent spectra and UC efficiency curves of emitter doped with different sensitizers. (a, b) PdOEP (10 μmol·L-1); (c, d) PdBrTPP(4 μmol·L-1), the fluorescence of Rh6G was set as the reference for the calculation of UC efficiency. The original data was shrank six times to fit the chart
    Fig. 12. Under excitation of 532 nm laser (400 mW·cm-2), the concentration-dependent spectra and UC efficiency curves of emitter doped with different sensitizers. (a, b) PdOEP (10 μmol·L-1); (c, d) PdBrTPP(4 μmol·L-1), the fluorescence of Rh6G was set as the reference for the calculation of UC efficiency. The original data was shrank six times to fit the chart
    Compd.λabs./nm
    Soret带
    λabs./nm
    Q带
    ε532 nm/
    (cm-1·mmol·L-1)
    λflu.
    /nm
    λphos.
    /nm
    ES1
    /eV
    ET1
    /eV
    ΔEST/eVτp
    /μs
    PdOEP391510, 5443.05956652.0821.8650.217109.21
    PdBrTPP41452210.86086942.0391.7870.252173.13
    Emitterλabs
    /nm
    λem
    /nm
    τf
    /ns
    Φf
    /%
    kf
    /(108 s-1)
    knf
    /(107 s-1)
    ES1
    /eV
    ET1
    /eV
    p-DHMPA337, 355
    373, 393
    412, 4305.9091.81.561.392.8841.725
    Table 1. Optical properitiesaod siglet/triplet energy levels of PdOEP, PdBrTPP and p-DHMPA in n-propanol
    SensitiserλUC
    /nm
    Euc-Eex
    /eV
    kq
    /(μmol·L-1·s-1)
    Ith
    /(mW·cm-2)
    ΦUC
    /%
    η
    /(cm-1·μmol·L-1)
    PdOEP4320.541.64×10-322.4028.30.849
    PdBrTPP4340.536.53×10-429.7826.82.894
    Table 2. Upconversion performance of PdOEP/p-DHMPAand PdBrTPP/p-DHMPA in n-propanol
    Chang-qing YE, Xue YU, Shuo-ran CHEN, Zuo-qin LIANG, Yu-yang ZHOU, Xiao-mei WANG. Study on the Structure/Energy-Level of Palladuim-Porphyrin Sensitizers on the Triplet-Triplet-Annihilation Upconversion Performance[J]. Spectroscopy and Spectral Analysis, 2021, 41(1): 71
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