拉曼光谱
拉曼散射
布里渊区
声子
G波段
分子物理学
带隙
图层(电子)
半导体
材料科学
谱线
X射线拉曼散射
单层
色散(光学)
分析化学(期刊)
化学
光学
凝聚态物理
光电子学
物理
纳米技术
天文
色谱法
作者
Biswanath Chakraborty,H. S. S. Ramakrishna Matte,A. K. Sood,C. N. R. Rao
摘要
We report resonant Raman scattering of MoS 2 layers comprising of single, bi, four and seven layers, showing a strong dependence on the layer thickness. Indirect band gap MoS 2 in bulk becomes a direct band gap semiconductor in the monolayer form. New Raman modes are seen in the spectra of single‐ and few‐layer MoS 2 samples which are absent in the bulk. The Raman mode at ~230 cm −1 appears for two, four and seven layers. This mode has been attributed to the longitudinal acoustic phonon branch at the M point (LA(M)) of the Brillouin zone. The mode at ~179 cm −1 shows asymmetric character for a few‐layer sample. The asymmetry is explained by the dispersion of the LA(M) branch along the Γ ‐M direction. The most intense spectral region near 455 cm −1 shows a layer‐dependent variation of peak positions and relative intensities. The high energy region between 510 and 645 cm −1 is marked by the appearance of prominent new Raman bands, varying in intensity with layer numbers. Resonant Raman spectroscopy thus serves as a promising non invasive technique to accurately estimate the thickness of MoS 2 layers down to a few atoms thick. Copyright © 2012 John Wiley & Sons, Ltd.
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