Shinde Nitin Babu, Eswaran Senthil Kumar
2D Materials and Devices Laboratory (2DML), Sir C. V. Raman Research Park, Department of Physics and Nanotechnology, SRM Institute of Science and Technology (SRMIST), Kattankulathur 603203, Chennai, India.
Nanotechnology Research Centre (NRC), SRM Institute of Science and Technology (SRMIST), Kattankulathur 603203, Chennai, India.
J Phys Chem Lett. 2021 Jul 8;12(26):6197-6202. doi: 10.1021/acs.jpclett.1c01795. Epub 2021 Jun 30.
Atomically thin MoS hosts rich and distinct vibrational spectral features, which are prominent under selective excitation energies near the excitonic transitions. In this work, we have investigated the resonant Raman scattering of the MoS layers of different thicknesses, from monolayer to five-layer samples, measured near resonance with the A excitonic transition. We show that the near-resonance excitation (1.96 eV) resulted in a Davydov splitting of the out-of-plane A-like phonon mode (A) around 406 cm caused by the weak interlayer interaction. The number of Davydov splitting components () equals the number of layers (NL) of the MoS, suggesting that it can be used as a thickness indicator. The origin of various Davydov components is understood based on a simple nearest-interlayer interaction. We extend our investigation to identify some acoustic phonon modes associated with characteristic second-order double-resonance Raman and disorder-induced bands.
原子级薄的二硫化钼(MoS)具有丰富且独特的振动光谱特征,这些特征在接近激子跃迁的选择性激发能量下尤为显著。在这项工作中,我们研究了从单层到五层样品的不同厚度MoS层的共振拉曼散射,测量是在与A激子跃迁接近共振的条件下进行的。我们表明,近共振激发(1.96电子伏特)导致由弱层间相互作用引起的面外类A声子模式(A)在约406厘米-1处出现达维多夫分裂。达维多夫分裂分量的数量()等于MoS的层数(NL),这表明它可作为厚度指示器。基于简单的最近层间相互作用可以理解各种达维多夫分量的起源。我们扩展研究以识别一些与特征二阶双共振拉曼和无序诱导带相关的声子模式。