夏云生, 戴洪兴, 何洪. 类球状和棒状Eu2O3和Sm2O3纳米粒子的合成与表征[J]. 北京工业大学学报, 2010, 36(1): 87-91.
    引用本文: 夏云生, 戴洪兴, 何洪. 类球状和棒状Eu2O3和Sm2O3纳米粒子的合成与表征[J]. 北京工业大学学报, 2010, 36(1): 87-91.
    XIA Yun-sheng, DAI Hong-xing, HE Hong. Fabrication and Characterization of Sphere-like and Rod-like Eu2O3 and Sm2O3 Nanoparticles[J]. Journal of Beijing University of Technology, 2010, 36(1): 87-91.
    Citation: XIA Yun-sheng, DAI Hong-xing, HE Hong. Fabrication and Characterization of Sphere-like and Rod-like Eu2O3 and Sm2O3 Nanoparticles[J]. Journal of Beijing University of Technology, 2010, 36(1): 87-91.

    类球状和棒状Eu2O3和Sm2O3纳米粒子的合成与表征

    Fabrication and Characterization of Sphere-like and Rod-like Eu2O3 and Sm2O3 Nanoparticles

    • 摘要: 采用表面活性剂和超声波辅助的沉淀法合成了类球状和棒状多晶Eu2O3和Sm2O3纳米粒子,并用透射电镜(TEM)、选区电子衍射(SAED)、X射线衍射(XRD)、N2吸附-脱附和紫外-可见漫反射(UV-Vis DRS)技术表征了其物理性质.结果表明,以十二烷基硫酸钠作表面活性剂所得产物为类球状体心立方晶相Eu2O3和单斜晶相Sm2O3纳米粒子,比表面积为44~49 m2/g;而以聚乙烯吡咯烷酮作表面活性剂所得产物则是棒状正交晶相Eu2O3和体心立方晶相Sm2O3纳米粒子,比表面积为34~37 m2/g.除了在紫外光区(λ<390 nm)有较强的吸收外,类球状和棒状Eu2O3和Sm2O3纳米粒子在可见光区(390 nm<λ<535 nm)也有不同程度的吸收.该吸光性能差异与所得稀土氧化物的表面形貌和晶体结构有关.

       

      Abstract: Sphere-like and rod-like Eu2O3 and Sm2O3 polycrystalline nanoparticles were fabricated by using a surfactant-and ultrasonic-assisted precipitation strategy.The physical properties of these nanomaterials were characterized by means of transmission electron microscopic(TEM),selected area electron diffraction(SAED),X-ray diffraction(XRD),nitrogen adsorption-desorption,and ultravioletvisible diffuse reflection spectroscopic(UV-Vis DRS) techniques.It is shown that the sphere-like body-centered cubic Eu2O3 and monoclinic Sm2O3 nanoparticles obtained with sodium dodecylsulfate as surfactant and the rod-like orthorhombic Eu2O3 and body-centered cubic Sm2O3 nanoparticles fabricated with polyvinylpyrrolidone as surfactant possessed a BET surface area of 44~49 and 34~37m2/g,respectively.In addition to a stronger absorption of UV light(λ<390nm),the sphere-like and rod-like Eu2O3 and Sm2O3 samples exhibited different absorption of visible light(390nm<λ<535nm).Such a difference in light absorption behavior might be a result due to various surface morphologies and crystal structures of the so-obtained rare earth oxides.

       

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