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Deep-ultraviolet Raman scattering spectroscopy of monolayer WS2

机译:单层WS2的深紫外拉曼散射光谱

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摘要

Raman scattering measurements of monolayer WS2 are reported as a function of the laser excitation energies from the near-infrared (1.58 eV) to the deep-ultraviolet (4.82 eV). In particular, we observed several strong Raman peaks in the range of 700∼850 cm−1 with the deep-ultraviolet laser lights (4.66 eV and 4.82 eV). Using the first-principles calculations, these peaks and other weak peaks were appropriately assigned by the double resonance Raman scattering spectra of phonons around the M and K points in the hexagonal Brillouin zone. The relative intensity of the first-order E2g1 to A1g peak changes dramatically with the 1.58 eV and 2.33 eV laser excitations, while the comparable relative intensity was observed for other laser energies. The disappearance of the E2g1 peak with the 1.58 eV laser light comes from the fact that valley polarization of the laser light surpasses the E2g1 mode since the E2g1 mode is the helicity-exchange Raman mode. On the other hand, the disappearance of the A1g peak with the 2.33 eV laser light might be due to the strain effect on the electron-phonon matrix element.
机译:据报道,单层WS2的拉曼散射测量结果是从近红外(1.58 eV)到深紫外光(4.82 eV)的激光激发能的函数。尤其是,在深紫外激光(4.66 eV和4.82 eV)下,我们在700〜850 cm -1 范围内观察到了几个很强的拉曼峰。使用第一性原理计算,这些峰和其他弱峰是由六边形布里渊区M和K点周围的声子的双共振拉曼散射光谱适当分配的。一阶 E 2 g 1 到A1g峰急剧变化,而相对强度却相当观察到其他激光能量。 E 2 g 1 峰来自于这样一个事实,即激光的谷底极化超过 E 2 g 1 模式,因为 E 2 g 1 模式就是螺旋度更改拉曼模式。另一方面,用2.33 eV激光使Al峰消失的原因可能是对电子-声子基体元素的应变作用。

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