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DUV Double-Resonant Raman Spectra and Interference Effect in Graphene: First-Principles Calculations
Zhang, Ye1,2; Liu, Renhui1,2; Huang, Jianqi3; Hung, Nguyen Tuan4; Saito, Riichiro5,6; Yang, Teng1,2; Zhang, Zhidong1,2
通讯作者Huang, Jianqi(jqhuang@lam.ln.cn) ; Yang, Teng(yanghaiteng@msn.com)
2025-01-13
发表期刊JOURNAL OF RAMAN SPECTROSCOPY
ISSN0377-0486
页码8
摘要We calculate double-resonance Raman (DRR) spectra of monolayer graphene by first-principles density functional calculation, for wide laser excitation energies from the near-infrared (1.58 eV) to the deep-ultraviolet (DUV, 5.41 eV) region. When laser excitation energy, EL$$ {E}_{\mathrm{L}} $$, goes into the DUV region, Raman peak wavenumber for G & lowast;$$ {}<^>{\ast } $$ band switches from red-shift to blue-shift and for 2D '$$ {}<^>{\prime } $$ band switches from red-shift to constant, in contrast to the continuous blue-shift of G '$$ {}<^>{\prime } $$ band. Raman intensity of the three bands generally decreases with increasing EL$$ {E}_{\mathrm{L}} $$, except for EL$$ {E}_{\mathrm{L}} $$ around 4.08 eV where Raman intensity diverges due to van Hove singularity of electron density of states. The combined two-phonon modes change with EL$$ {E}_{\mathrm{L}} $$ for both G '$$ {}<^>{\prime } $$ and G & lowast;$$ {}<^>{\ast } $$ bands (e.g., from 2LO to 2TO and back to 2LO for G '$$ {}<^>{\prime } $$ and from LA + LO/TO to TA + LO/TO for G & lowast;$$ {}<^>{\ast } $$) but remain 2LO for 2D '$$ {}<^>{\prime } $$ band. Further, the dominant DRR scattering process of G '$$ {}<^>{\prime } $$ band changes from the electron-hole (eh$$ eh $$ or he$$ he $$) scattering processes to the ee$$ ee $$ scattering processes as EL$$ {E}_{\mathrm{L}} $$ goes into the DUV region, since the Dirac energy bands become asymmetric between pi$$ \pi $$ and pi & lowast;$$ {\pi}<^>{\ast } $$ band that suppresses the eh$$ eh $$ process and the Raman intensity. Another factor to suppress the Raman intensity is the quantum interference effect between four scattering processes (eh,he,ee,hh$$ eh, he, ee, hh $$) which changes from constructive to destructive interference and finally to no interference with increasing EL$$ {E}_{\mathrm{L}} $$. We calculate EL$$ {E}_{\mathrm{L}} $$-dependent Raman tensor of the three bands and polarized Raman spectra, which further support the interference effect. The calculated results are directly compared and consistent with the experimental results.
资助者National Natural Science Foundation of China ; National Key R&D Program of China ; JSPS KAKENHI grant ; Ministry of Education (MOE), Taiwan ; Frontier Research Institute for Interdisciplinary Sciences, Tohoku University
DOI10.1002/jrs.6768
收录类别SCI
语种英语
资助项目National Natural Science Foundation of China ; National Key R&D Program of China[2022YFA1203900] ; JSPS KAKENHI grant[JP22H00283] ; Ministry of Education (MOE), Taiwan ; Frontier Research Institute for Interdisciplinary Sciences, Tohoku University ; [12404213] ; [52031014]
WOS研究方向Spectroscopy
WOS类目Spectroscopy
WOS记录号WOS:001395475700001
出版者WILEY
引用统计
文献类型期刊论文
条目标识符http://ir.imr.ac.cn/handle/321006/180859
专题中国科学院金属研究所
通讯作者Huang, Jianqi; Yang, Teng
作者单位1.Chinese Acad Sci, Inst Met Res, Shenyang Natl Lab Mat Sci, Shenyang, Peoples R China
2.Univ Sci & Technol China, Sch Mat Sci & Engn, Shenyang, Peoples R China
3.Liaoning Acad Mat, Shenyang, Peoples R China
4.Tohoku Univ, Frontier Res Inst Interdisciplinary Sci, Sendai, Japan
5.Natl Taiwan Normal Univ, Dept Phys, Taipei, Taiwan
6.TOHOKU UNIV, DEPT PHYS, SENDAI, Japan
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GB/T 7714
Zhang, Ye,Liu, Renhui,Huang, Jianqi,et al. DUV Double-Resonant Raman Spectra and Interference Effect in Graphene: First-Principles Calculations[J]. JOURNAL OF RAMAN SPECTROSCOPY,2025:8.
APA Zhang, Ye.,Liu, Renhui.,Huang, Jianqi.,Hung, Nguyen Tuan.,Saito, Riichiro.,...&Zhang, Zhidong.(2025).DUV Double-Resonant Raman Spectra and Interference Effect in Graphene: First-Principles Calculations.JOURNAL OF RAMAN SPECTROSCOPY,8.
MLA Zhang, Ye,et al."DUV Double-Resonant Raman Spectra and Interference Effect in Graphene: First-Principles Calculations".JOURNAL OF RAMAN SPECTROSCOPY (2025):8.
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