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Low Temperature Growth of Hydrogenated Silicon Prepared by PECVD from Argon Diluted Silane Plasma

机译:PECVD氩稀释硅烷等离子体低温制备氢化硅

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In order to contribute to the understanding of the optoelectronics properties of hydrogenated nanocrystalline silicon thin films, a detailed study has been conducted. The samples were deposited by 13.56 MHz PECVD (Plasma-Enhanced Chemical Vapor Deposition) of silane argon mixture. The argon dilution of silane for all samples studied was 96% by volume. The substrate temperature was fixed at 200oC. The influence of depositions parameters on optical proprieties of samples was studied by UV-Vis-NIR spectroscopy. The structural evolution was studied by Raman spectroscopy and X-ray diffraction (XRD). Intrinsic-layer samples depositions were made in this experiment in order to obtain the transition from the amorphous to crystalline phase materials. The deposition pressure varied from 400 mTorr to 1400 mTorr and the rf power from 50 to 250 W. The structural evolution studies show that beyond 200 W, we observed an amorphous-nanocrystalline transition, with an increase in crystalline fraction by increasing rf power and working pressure. Films near the amorphous to nanocrystalline transition region are grown at reasonably high deposition rates (~10 /s), which are highly desirable for the fabrication of cost effective devices. The deposition rate increases with increasing rf power and process pressure. Different crystalline fractions (21% to 95%) and crystallite size (6 - 16 nm) can be achieved by controlling the process pressure and rf power. These structural changes are well correlated to the variation of optical proprieties of the thin films.
机译:为了有助于理解氢化纳米晶硅薄膜的光电特性,已经进行了详细的研究。通过13.56 MHz的硅烷氩气混合物的PECVD(等离子体增强化学气相沉积)沉积样品。对于所有研究的样品,硅烷的氩气稀释量为96%(体积)。基板温度固定为200oC。通过紫外-可见-近红外光谱研究了沉积参数对样品光学性能的影响。通过拉曼光谱和X射线衍射(XRD)研究了结构演变。为了获得从非晶相到结晶相材料的过渡,在本实验中进行了本征层样品沉积。沉积压力从400 mTorr到1400 mTorr不等,rf功率从50到250 W不等。结构演变研究表明,超过200 W,我们观察到非晶-纳米晶转变,随着rf功率和工作量的增加,晶体分数增加压力。非晶态到纳米晶过渡区域附近的薄膜以合理的高沉积速率(〜10 / s)生长,这对于制造经济高效的器件非常有用。沉积速率随着射频功率和工艺压力的增加而增加。通过控制工艺压力和射频功率,可以实现不同的晶体分数(21%至95%)和微晶尺寸(6-16 nm)。这些结构变化与薄膜的光学特性的变化密切相关。

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