Double resonance Raman spectroscopy of single-wall carbon nanotubes
By Riichiro Saito, A. Grüneis, Georgii Samsonidze, V. Brar, G. Dresselhaus, Mildred S. Dresselhaus, A. Jorio, Luiz Gustavo Cançado, C. Fantini, M. Pimenta and 1 more. 2003
243 citations recorded by the source corpus.
A review of double resonance Raman spectroscopy is presented. Non-zone centre phonon modes in solids can be observed in the double resonance Raman spectra, in which weak Raman signals appear in a wide frequency region and their combination or overtone modes can be assigned. By changing the excitation laser energy, we can derive the phonon dispersion relations of a single nanotube.
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Citations in the corpus
- G' band Raman spectra of single, double and triple layer graphene (2009, methodology): “[9] Saito R, Gruneis A, Samsonidze GG, Brar VW, Dresselhaus G, Dresselhaus MS, et al.”
- Comparative study of first- and second-order Raman spectra of MWCNT at visible and infrared laser excitation (2006, background): “The explanation for this is based on resonances with van Hove singularities [18].”
- Raman spectroscopy of carbon nanotubes (2005, background): “Hereafter we call them, respectively, one- and two-phonon double-resonance Raman spectra [21].”
- Raman Spectra of Carbon-Based Materials (from Graphite to Carbon Black) and of Some Silicone Composites (2015, background): “Hence, as a consequence of the particular shape and symmetry of the π and π* electronic states around the K point of the Brillouin zone, the energy and momentum transfer of the resonant phonons vary according to the slope of the dispersion branches involved in the double resonance process [38,41–44]”