2018
DOI: 10.1016/j.dyepig.2018.02.044
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Bright white-light upconversion from core-shell nanocrystals through interfacial energy transfer

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Cited by 16 publications
(6 citation statements)
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“…Because the 1 S 0 → 3 P 1 transition of Bi 3+ (260 nm) is more intense than the CTB (230 nm), the 260 nm is the most efficient excitation wavelength for (Y 0.95-x Eu 0.05 Bi x )BO 3 spheres. Under excitation at 260 nm, the emission spectra show emission peaks at~592 nm, 610 and~627 nm,~650 and~673 nm, and~694 and~708 nm, which are assigned to the typical 5 D 0 → 7 F J (J = 1,2,3,4) transition of Eu 3+ ions respectively [26] (Figure 4(b)). Because activator Eu 3+ occupies the Y 3+ site in hexagonal structure with the point symmetry of S 6 , the magnetic dipole 5 D 0 → 7 F 1 transition of Eu 3+ at 592 nm takes the dominate role, rather than the forced electric dipole 5 D 0 → 7 F 2 transition of Eu 3+ ions at~610 and~627 nm [12][13][14][15][16].…”
Section: Morphology and Phase Structurementioning
confidence: 99%
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“…Because the 1 S 0 → 3 P 1 transition of Bi 3+ (260 nm) is more intense than the CTB (230 nm), the 260 nm is the most efficient excitation wavelength for (Y 0.95-x Eu 0.05 Bi x )BO 3 spheres. Under excitation at 260 nm, the emission spectra show emission peaks at~592 nm, 610 and~627 nm,~650 and~673 nm, and~694 and~708 nm, which are assigned to the typical 5 D 0 → 7 F J (J = 1,2,3,4) transition of Eu 3+ ions respectively [26] (Figure 4(b)). Because activator Eu 3+ occupies the Y 3+ site in hexagonal structure with the point symmetry of S 6 , the magnetic dipole 5 D 0 → 7 F 1 transition of Eu 3+ at 592 nm takes the dominate role, rather than the forced electric dipole 5 D 0 → 7 F 2 transition of Eu 3+ ions at~610 and~627 nm [12][13][14][15][16].…”
Section: Morphology and Phase Structurementioning
confidence: 99%
“…The shortened lifetime of Bi 3+ emission at higher Eu content (Figure 7(b) and Figure S2) confirms the energy transfer process from Bi 3+ to Tb 3+ and Eu 3+ . In the absence of concentration quenching, the efficiency (η ET ) of the Bi 3+ → "Eu 3+ and Tb 3+ " energy transfer can be calculated from the fluorescence lifetime with η ET = 1-τ/τ 0 , where τ and τ 0 are the fluorescence lifetime of the Bi 3+ emission in the presence and absence of the acceptor [18,26]. The η TE value, calculated from Figure 7(b), gradually increases from 2% for y = 0.01 to 63% for y = 0.09.…”
Section: Luminescence Behavior Of (Y Tb Eu Bi)bo 3 Spheresmentioning
confidence: 99%
“…However, current researches mainly focus on the occurrence level of the IET phenomenon in core−shell structure, and the objects that are usually compared either do not have the core−shell structure or there is no occurrence of IET phenomenon. 35 In addition, in these reports, some of them doped sensitizer ions into the shell and activator ions into the core, and some of them doped sensitizer ions into the core and activator ions into the shell, 36 and so far, there has been no comparative study on the two cases.…”
Section: Introductionmentioning
confidence: 99%
“…Zhou et al achieved upconversion of photons and accurate control of donor–acceptor interactions via interfacial energy transfer . Tao et al applied the interfacial energy transfer method to core–shell structures and proved a new white light emission upconversion strategy . Zhou et al realized enhancing multiphoton upconversion by interfacial energy transfer in multilayered nanoparticles .…”
Section: Introductionmentioning
confidence: 99%
“…20 Tao et al applied the interfacial energy transfer method to core−shell structures and proved a new white light emission upconversion strategy. 21 multilayered nanoparticles. 22 Wang et al synthesized hollow double-shelled TiO 2 :x%Eu 3+ @SiO 2 :y%Tb 3+ nanospheres and analyzed the mechanism of interfacial energy transfer.…”
Section: Introductionmentioning
confidence: 99%