Dong Xiao, Wang Yongyong, Song Xiaohui
College of Physics and Materials Science, Henan Normal University, 453007 Xinxiang, People's Republic of China. Henan Key Laboratory of Photovoltaic Materials, 453007 Xinxiang, People's Republic of China.
J Phys Condens Matter. 2020 Mar 13;32(11):115701. doi: 10.1088/1361-648X/ab5901. Epub 2019 Nov 19.
The Raman spectra difference of the N-hyperdoped silicon prepared under different conditions is due to the different dominant configurations of N in silicon. The separate substitutional N atoms in silicon show several strong Raman peaks which can be also observed in the chalcogen-hyperdoped silicon. The configuration with separate substitutional and interstitial N atoms displays a strong and broad Raman band at 480 cm, which is in accordance with our experiment. The introduction of the vacancies may lead to the disappearance or appearance of the Raman peaks, which depends on the dominant configurations of the N atoms. For the compound of interstitial N atoms and vacancies, the calculational Raman spectrum is similar to that of the NF-prepared silicon and N-prepared silicon with a lower laser power.
不同条件下制备的氮超掺杂硅的拉曼光谱差异源于氮在硅中的不同主导构型。硅中单独的替代氮原子显示出几个很强的拉曼峰,这在硫族元素超掺杂硅中也能观察到。单独的替代氮原子和间隙氮原子的构型在480 cm处显示出一个强而宽的拉曼带,这与我们的实验结果一致。空位的引入可能导致拉曼峰的消失或出现,这取决于氮原子的主导构型。对于间隙氮原子和空位的化合物,计算得到的拉曼光谱与用较低激光功率制备的NF硅和N硅的拉曼光谱相似。