周期性硅纳米结构的光学和电子性质

A. Tavkhelidze, A. Bayramov, Y. Aliyeva, L. Jangidze, G. Skhiladze, S. Asadullayeva, O. Alekperov, N. Mamedov
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引用次数: 4

摘要

采用激光干涉光刻技术在Si/SiO2/衬底器件结构的顶部Si层表面制备了纳米光栅。然后研究了普通Si和纳米Si结构上的电子输运、光致发光和拉曼散射,以观察纳米Si引入的影响。由于引入了NG并很可能维持了g掺杂,本研究中研究的所有样品都显示出NG Si的电阻率降低了2到3个数量级。霍尔系数表明电子是g掺杂的主要载流子。在532 nm (2.38 eV)和325 nm (3.81 eV)的激光激发下,普通硅层均无光致发光现象。在光子能量在1.5 ~ 3.5 eV之间的ngsi层上观察到由多个几乎等距峰组成的宽光致发光带。在室温下观察到了522.65 cm−1声子的Stocks和anti-Stocks分量。根据Stocks和anti-Stocks分量强度之比估计,声子气体温度在环境温度(295 K)以下的下降(如果有的话)不超过3 K。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Optical and electronic properties of periodic Si nanostructures
Nanogratings (NGs) on the surface of the top Si layer of a Si/SiO2/ substrate device structure were prepared using laser interference lithography. Electron transport, photoluminescence, and Raman scattering were then studied on the plain Si and NG Si structures to see the effect of NG introduction. As a result of NG-introduction and very likely G-doping maintenance, all samples studied in this work displayed a 2 to 3 order of magnitude reduction in resistivity for NG Si. The Hall coefficient indicated that electrons are main charge carriers that is also expected for exactly G-doping. Plain Si layer did not show any photoluminescence either for 532 nm (2.38 eV) or 325 nm (3.81 eV) laser excitation. A broad photoluminescence band, composed of a number of almost equidistant peaks was observed on NG Si layer between the photon energies 1.5 and 3.5 eV. Both Stocks and anti-Stocks components for 522.65 cm−1 phonons at room temperature were observed in the Raman spectra of NG Si layer. Estimated from the ratio between the intensities of Stocks and anti-Stocks components, the drop (if any) in phonon gas temperature below ambient (295 K) does not exceed 3 K.
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