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首页> 外文期刊>The European physical journal, D. Atomic, molecular, and optical physics >Synthesis and characterization of Cd_(1?x)Zn_xS nanopowder and its nanostructured thin films
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Synthesis and characterization of Cd_(1?x)Zn_xS nanopowder and its nanostructured thin films

机译:Cd_(1?x)Zn_xS纳米粉体及其纳米结构薄膜的合成与表征

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摘要

Cd_(1?x)Zn_xS (with x = 0, 0.01, 0.03, 0.05 and 0.1) nanopowder were synthesized by chemical precipitation method under N_2 atmosphere at room temperature. Cd_(1?x)Zn_xS nanostructured thin films were deposited on the glass at 450 ?C by spraying the colloidal suspension of the Cd_(1?x)Zn_xS nanoparticles. Optical and structural properties of both nanostructures were investigated. The prominent peaks of X-ray diffractions (XRD) of samples indicate that the Cd_(1?x)Zn_xS crystalline grain size in the nanostructured thin film is larger than the Cd_(1?x)Zn_xS nanoparticles in the nanopowder, due to growing of the grains, originated from high temperature of the substrate. UV-Vis absorption spectra show that both Cd_(1?x)Zn_xS nanostructures have smaller band edge wavelength in comparison with bulk samples. There is also an increase in blue shift value of the band gap of both Cd_(1?x)Zn_xS nanostructures, with increasing x, which can be attributed to Burstein-Moss effect. It was found that the variation of the band gap of ZnxCd1?xS nanopowder and nanostructured thin films with Zn concentration are approximately linear with similar slopes. Photoluminescence (PL) spectra indicated that the emission peaks of both the samples are shifted toward the shorter wavelengths with increasing Zn~(+2) ions.
机译:在室温N_2气氛下,通过化学沉淀法合成了Cd_(1?x)Zn_xS(x = 0,0.01,0.03,0.05和0.1)纳米粉。通过喷涂Cd_(1?x)Zn_xS纳米颗粒的胶体悬浮液,在450°C的玻璃上沉积Cd_(1?x)Zn_xS纳米结构薄膜。研究了两种纳米结构的光学和结构性质。样品的X射线衍射(XRD)的突出峰表明,由于生长,纳米结构薄膜中的Cd_(1?x)Zn_xS晶体晶粒尺寸大于纳米粉中的Cd_(1?x)Zn_xS纳米颗粒。晶粒的一部分是由于基材的高温引起的。 UV-Vis吸收光谱表明,与大量样品相比,两种Cd_(1?x)Zn_xS纳米结构均具有更小的带边缘波长。两个Cd_(1?x)Zn_xS纳米结构的带隙的蓝移值也随着x的增加而增加,这可以归因于Burstein-Moss效应。结果表明,ZnxCd1?xS纳米粉体和带Zn浓度的纳米结构薄膜的带隙变化近似线性,且斜率相似。光致发光(PL)光谱表明,随着Zn〜(+2)离子的增加,两个样品的发射峰都向较短的波长移动。

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