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用于碳纳米管和二维材料的深紫外与螺旋度相关拉曼光谱

Deep-Ultraviolet and Helicity-Dependent Raman Spectroscopy for Carbon Nanotubes and 2D Materials.

作者信息

Saito Riichiro, Hung Nguyen Tuan, Yang Teng, Huang Jianqi, Liu Hsiang-Lin, Gulo Desman Perdamaian, Han Shiyi, Tong Lianming

机构信息

Department of Physics, National Taiwan Normal University, Taipei, 11677, Taiwan.

Department of Physics, and Tohoku University, Sendai, 980-8578, Japan.

出版信息

Small. 2025 Jul;21(28):e2308558. doi: 10.1002/smll.202308558. Epub 2024 Feb 27.

Abstract

Recent progress of Raman spectroscopy on carbon nanotubes and 2D materials is reviewed as a topical review. The Raman tensor with complex values is related to the chiral 1D/2D materials without mirror symmetry for the mirror in the propagating direction of light, such as chiral carbon nanotube and black phosphorus. The phenomenon of complex Raman tensor is observed by the asymmetric polar plot of helicity-dependent Raman spectroscopy using incident circularly-polarized lights. First-principles calculations of resonant Raman spectra directly give the complex Raman tensor that explains helicity-dependent Raman spectra and laser-energy-dependent relative intensities of Raman spectra. In deep-ultraviolet (DUV) Raman spectroscopy with 266 nm laser, since the energy of the photon is large compared with the energy gap, the first-order and double resonant Raman processes occur in general k points in the Brillouin zone. First-principles calculation is necessary to understand the DUV Raman spectra and the origin of double-resonance Raman spectra. Asymmetric line shapes appear for the G band of graphene for 266 nm laser and in-plane Raman mode of WS for 532 nm laser, while these spectra show symmetric line shapes for other laser excitation. The interference effect on the asymmetric line shape is discussed by fitting the spectra to the Breit-Wigner-Fano line shapes.

摘要

作为一篇专题综述,本文回顾了拉曼光谱在碳纳米管和二维材料方面的最新进展。对于光传播方向上无镜面反射对称性的手性一维/二维材料,如手性碳纳米管和黑磷,具有复数值的拉曼张量与之相关。通过使用入射圆偏振光的螺旋度相关拉曼光谱的不对称极坐标图,可以观察到复拉曼张量现象。共振拉曼光谱的第一性原理计算直接给出了复拉曼张量,它解释了螺旋度相关拉曼光谱以及拉曼光谱的激光能量相关相对强度。在使用266nm激光的深紫外(DUV)拉曼光谱中,由于光子能量与能隙相比很大,一阶和双共振拉曼过程通常发生在布里渊区的一般k点。理解DUV拉曼光谱和双共振拉曼光谱的起源需要进行第一性原理计算。对于266nm激光作用下的石墨烯G带以及532nm激光作用下的WS面内拉曼模式,会出现不对称线形,而对于其他激光激发,这些光谱呈现对称线形。通过将光谱拟合为Breit-Wigner-Fano线形来讨论不对称线形的干涉效应。

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