Colloidal synthesis and blue based multicolor upconversion emissions of size and composition controlled monodisperse hexagonal NaYF4 : Yb,Tm nanocrystals

光子上转换 纳米晶 材料科学 作文(语言) 胶体 分散性 化学工程 兴奋剂 六方晶系 光电子学 纳米技术 化学 结晶学 工程类 语言学 哲学 高分子化学
作者
Anxiang Yin,Ya‐Wen Zhang,Ling‐Dong Sun,Chun‐Hua Yan
出处
期刊:Nanoscale [The Royal Society of Chemistry]
卷期号:2 (6): 953-953 被引量:231
标识
DOI:10.1039/b9nr00397e
摘要

Monodisperse β-NaYF4 : Yb,Tm nanocrystals with controlled size (25–150 nm), shape (sphere, hexagonal prism, and hexagonal plate), and composition (Yb: 20–40%, Tm: 0.2–5%) were synthesized from the thermolysis of metal trifluoroacetates in hot surfactant solutions. The upconversion (UC) of near-infrared light (980 nm) to ultra-violet (360 nm), blue (450 and 475 nm), red (650 and 695 nm) and infrared (800 nm) light in the β-NaYF4 : Yb,Tm nanocrystals has been studied by UC spectroscopy. Both the total intensity of UC emissions and the relative intensities of emissions at different wavelengths have shown a strong dependence on different particle sizes and different Tm3+ and Yb3+ concentrations. As a result, different overall output colors of UC emissions can be achieved by altering sizes and Yb3+/Tm3+ doping concentrations of the β-NaYF4 : Yb,Tm nanocrystals. The intensity-power curves of a series of samples have proved that emissions at 360 and 450 nm can be ascribed to four-photon process (1D2 to 3H6 and 1D2 to 3H4, respectively), while emissions at 475 and 650 nm are three-photon processes (1G4 to 3H6 and 1G4 to 3H4, respectively) and emissions at 695 and 800 nm are two-photon ones (3F2 to 3H6 and 3F4 to 3H6, respectively). A UC saturation effect would occur under a certain excitation intensity of the 980 nm CW diode laser for the as-obtained β-NaYF4 : Yb,Tm nanocrystals, leading to the decrease of the slopes of the I–P curves. The results of our study also revealed that the successive transfer model instead of the cooperative sensitization model can be applied to explain the UC behaviors of the β-NaYF4 : Yb,Tm nanocrystals. Further, an unexpected stronger emissions of four-photon process at 360 and 450 nm for ∼50 nm β-NaYF4 : Yb,Tm nanocrystals than those for the bigger (∼150 nm) nanocrystals was observed and explained in terms of the effects of crystallite size, surface-to-volume ratio and homogeneity of the doping cations.
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