中国物理B ›› 2025, Vol. 34 ›› Issue (6): 66301-066301.doi: 10.1088/1674-1056/adc36e
Weidong Wang(王卫东)1, Renhui Liu(刘仁辉)2,3, Ye Zhang(张也)2,3, Huaihong Guo(郭怀红)1,†, Jianqi Huang(黄建啟)4,‡, Zhantong Liu(刘展彤)1, Heting Zhao(赵贺霆)1, Kai Wang(王凯)1, Bo Zhao(赵波)1, and Teng Yang(杨腾)2,3,§
Weidong Wang(王卫东)1, Renhui Liu(刘仁辉)2,3, Ye Zhang(张也)2,3, Huaihong Guo(郭怀红)1,†, Jianqi Huang(黄建啟)4,‡, Zhantong Liu(刘展彤)1, Heting Zhao(赵贺霆)1, Kai Wang(王凯)1, Bo Zhao(赵波)1, and Teng Yang(杨腾)2,3,§
摘要: MoS$_2$ monolayer, as a highly promising two-dimensional semiconducting material for electronic and optoelectronic applications, exhibits deep-ultraviolet (DUV) laser-induced anomalous lattice dynamics as revealed by Raman spectroscopy. Remarkably, not only the Raman intensity of many second-order Raman peaks but also the intensity ratio between the first-order modes $E'$ and $A_{1}'$ exhibits a non-monotonic behavior that depends on laser energy. Moreover, there are significant inconsistencies in the literature regarding the assignments of these second-order Raman modes. In this work, we perform a thorough exploration of the anomalous lattice dynamics and conduct a renewed assignment of the numerous double resonant Raman modes of MoS$_2$ monolayer. At three laser energies ($E_{\rm{L}} = 2.33$, 3.50, and 4.66 eV) spanning from the visible to the ultraviolet and further into the DUV region, the calculated double-resonance Raman spectra correlate reasonably well with the experimental ones in terms of both peak positions and relative intensities. We confirm that the $P_{\rm{1}}$ peak at $\sim 450 $ cm$^{-1}$ represents the second-order longitudinal acoustic (2$LA$) overtone mode. Each of the $P_{{i}}$ ($i = 1$, 2, $\ldots$, 7) peaks has multiple contributions from two phonons with distinct $q$ wavevectors. Our calculations further reveal that the DUV laser-induced anomalous lattice dynamics stems from the quantum interference effect among different Raman scattering channels.
中图分类号: (First-principles theory)