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Resonant Raman scattering of anthracene-based carbons in the secondary carbonization stage O. A. Maslova, M. R. Ammar, C. Fantini [et al.]

Contributor(s): Maslova, Olga A | Ammar, Mohamed Ramzi | Fantini, Cristiano | Barannikova, Svetlana A, 1971- | Pimenta, Marcos AssunçãoMaterial type: ArticleArticleContent type: Текст Media type: электронный Subject(s): резонансное комбинационное рассеяние | углерод | антрацен | карбонизацияGenre/Form: статьи в журналах Online resources: Click here to access online In: Journal of Raman spectroscopy Vol. 52, № 3. P. 670-677Abstract: The Raman spectra of graphene-based matter exhibit a set of defect/disorder-induced bands. The D band, which exhibits a strong dispersion up to similar to 50 cm(-1)/eV, comes from transverse optical phonons around K or K ' in the first Brillouin zone and involves an intervalley double resonance (DR) Raman process. In the present work, resonant Raman scattering (lines ranging from 1.58 to 3.81 eV) is used to study the unusual behavior of the one-phonon Raman band of a carbonaceous material (anthracene-based carbon which is one of the graphitizable carbons) upon its secondary carbonization stage (450 degrees C-1000 degrees C). While the G band appears to be nondispersive, the D band exhibits a change in both position and intensity. Its dispersion progressively rises from similar to 6 cm(-1)/eV to values close to what is usually observed in defected graphene-based systems when anthracene-based carbon becomes almost pure. This evolution appears to be correlated with a release of hydrogen (fixed on the edges of polyaromatic layers) questioning their role in changing the D band resonance conditions.
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The Raman spectra of graphene-based matter exhibit a set of defect/disorder-induced bands. The D band, which exhibits a strong dispersion up to similar to 50 cm(-1)/eV, comes from transverse optical phonons around K or K ' in the first Brillouin zone and involves an intervalley double resonance (DR) Raman process. In the present work, resonant Raman scattering (lines ranging from 1.58 to 3.81 eV) is used to study the unusual behavior of the one-phonon Raman band of a carbonaceous material (anthracene-based carbon which is one of the graphitizable carbons) upon its secondary carbonization stage (450 degrees C-1000 degrees C). While the G band appears to be nondispersive, the D band exhibits a change in both position and intensity. Its dispersion progressively rises from similar to 6 cm(-1)/eV to values close to what is usually observed in defected graphene-based systems when anthracene-based carbon becomes almost pure. This evolution appears to be correlated with a release of hydrogen (fixed on the edges of polyaromatic layers) questioning their role in changing the D band resonance conditions.

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