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首页> 外文期刊>Applied Physics >Evaluation of optoelectronic response and Raman active modes in Tb~(3+) and Eu~(3+) -doped gadolinium oxide (Gd_2O_3) nanoparticle systems
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Evaluation of optoelectronic response and Raman active modes in Tb~(3+) and Eu~(3+) -doped gadolinium oxide (Gd_2O_3) nanoparticle systems

机译:Tb〜(3+)和Eu〜(3+)掺杂的氧化g(Gd_2O_3)纳米粒子系统中的光电响应和拉曼激活模式的评估

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摘要

Rare earth oxide (Tb~(3+):Gd_2O_3 and Eu~(3+):Gd_2O_3) nanophosphors are exploited through spectroscopic and microscopic tools with special emphasis on D-F mediated radiative emission and Raman active vibrational modes. Powder X-ray diffraction measurements have revealed cubic crystal structure of the nanosystems and with an average crystallite size varying between ~3.2 and 4.8 nm. Photoluminescence (PL) spectra of Tb~(3+) doped systems signify intense blue-green (~490nm) and green (~ 544 nm) emissions mediated by ~5D_4 → ~7F_6 and ~5D_4 → ~7F_5 transitional events; respectively. In the PL responses of Eu~(3+) doped nanoparticle systems, we also identify magnetically-driven ~5D_0 → ~7F_1 (~591 nm) and electrically driven ~5D_0 → ~7F_2 (~619 nm) radiative features which seem to improve with increasing doping level. However, the magnitude of Judd-Ofelt (J-O) intensity parameters (Ω_(2, 4)), is significantly lowered for the high doping cases. Raman spectra of the undoped and RE doped systems exhibited several A_g and F_g modes in the range of Raman shift ~ 100-600 cm~(-1). In the Raman spectra, the peaks located at ~355 cm~(-1) are assigned to the mixed mode of F_g + A_g, the line width of which was found to increase with RE doping. Moreover, owing to the enhanced defect concentration in the doped systems than its undoped counterpart, we anticipate a faster phonon relaxation and consequently, a suppression of phonon lifetime in the former case.
机译:稀土氧化物(Tb〜(3 +):Gd_2O_3和Eu〜(3 +):Gd_2O_3)纳米磷光体是通过光谱和显微工具开发的,特别着重于D-F介导的辐射发射和拉曼主动振动模式。粉末X射线衍射测量显示出纳米系统的立方晶体结构,平均微晶尺寸在〜3.2至4.8 nm之间变化。 Tb〜(3+)掺杂系统的光致发光(PL)光谱表示由〜5D_4→〜7F_6和〜5D_4→〜7F_5过渡事件介导的强烈蓝绿色(〜490nm)和绿色(〜544 nm)发射;分别。在Eu〜(3+)掺杂的纳米粒子系统的PL响应中,我们还发现了磁驱动的〜5D_0→〜7F_1(〜591 nm)和电驱动的〜5D_0→〜7F_2(〜619 nm)辐射特征,这些辐射特征似乎有所改善随着掺杂水平的提高。但是,对于高掺杂情况,贾德-奥费尔特(J-O)强度参数(Ω_(2,4))的幅度明显降低。未掺杂和稀土​​掺杂体系的拉曼光谱在拉曼位移〜100-600 cm〜(-1)范围内表现出几种A_g和F_g模式。在拉曼光谱中,位于〜355 cm〜(-1)处的峰属于F_g + A_g的混合模式,发现其线宽随RE掺杂而增加。此外,由于掺杂体系中的缺陷浓度比未掺杂体系中的缺陷浓度提高,我们预计声子弛豫更快,因此,在前一种情况下,声子寿命受到抑制。

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  • 来源
    《Applied Physics》 |2016年第9期|845.1-845.10|共10页
  • 作者

    Nibedita Paul; D. Mohanta;

  • 作者单位

    Department of Physics, National Institute of Technology Nagaland, Chumukedima, Dimapur, Nagaland 797103, India,Department of Physics, Tezpur University, Napaam, Tezpur, Assam 784 028, India;

    Department of Physics, Tezpur University, Napaam, Tezpur, Assam 784 028, India;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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  • 正文语种 eng
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