4.8 Article

Raman Linewidth Contributions from Four-Phonon and Electron-Phonon Interactions in Graphene

Journal

PHYSICAL REVIEW LETTERS
Volume 128, Issue 4, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevLett.128.045901

Keywords

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Funding

  1. U.S. National Science Foundation [2015946, 2015954]
  2. Natural Science Foundation of China (NSFC) [12004254]
  3. GuangDong Basic and Applied Basic Research Foundation [2021A1515010042]
  4. Stable Support Plan of the Higher Education Institutions of Shenzhen [20200809161605001]
  5. NSFC [12174261]
  6. Directorate For Engineering
  7. Div Of Chem, Bioeng, Env, & Transp Sys [2015946] Funding Source: National Science Foundation
  8. Div Of Chem, Bioeng, Env, & Transp Sys
  9. Directorate For Engineering [2015954] Funding Source: National Science Foundation

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This study considers multiple factors such as phonon anharmonicity, phonon renormalization, and electron-phonon coupling on the Raman peak frequency shift and linewidth in graphene samples. The results show that four-phonon scattering contributes significantly to the linewidth, increasing with temperature, while the temperature dependence of electron-phonon interactions reverses above a certain doping threshold.
The Raman peak position and linewidth provide insight into phonon anharmonicity and electron-phonon interactions in materials. For monolayer graphene, prior first-principles calculations have yielded decreasing linewidth with increasing temperature, which is opposite to measurement results. Here, we explicitly consider four-phonon anharmonicity, phonon renormalization, and electron-phonon coupling, and find all to be important to successfully explain both the G peak frequency shift and linewidths in our suspended graphene sample over a wide temperature range. Four-phonon scattering contributes a prominent linewidth that increases with temperature, while temperature dependence from electron-phonon interactions is found to be reversed above a doping threshold (PLANCK CONSTANT OVER TWO PI omega(G)/2, with omega(G) being the frequency of the G phonon).

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