Characterizing carbon nanotube samples with resonance Raman scattering

By A. Jorio, M. Pimenta, Antônio Gomes Souza Filho, R. Saito, G. Dresselhaus, Mildred S. Dresselhaus. 2003

980 citations recorded by the source corpus.

The basic concepts and characteristics of Raman spectra from carbon nanotubes (both isolated and bundled) are presented. The general characteristics of the radial breathing mode, tangential mode (G band), disorder-induced mode (D-band) and other Raman features are presented, with the focus directed toward their use for carbon nanotube characterization. Polarization analysis, surface enhanced Raman spectroscopy and complementary optical techniques are also discussed in terms of their advantages and limitations.

Subfields: Materials Chemistry

View Paper: https://www.semanticscholar.org/paper/493b8c143785c20f8926a5b9979e106cd36ad39c

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In Materials Chemistry

1. A. Jorio
2. Mildred S. Dresselhaus
3. R. Saito
4. G. Dresselhaus
5. L. Bokobza
6. J. Zhang
7. M. Couzi
8. J. Bruneel

Citations in the corpus

• Raman spectroscopic characterization of multiwall carbon nanotubes and of composites (2012, methodology): “ful and nondestructive technique for the characterization of carbon-based materials including carbon black (CB) and carbon nanotubes (CNTs) and it has become an invaluable tool for understanding many fundamental aspects of all sp2 carbons [7, 8].”
• Mixed surfactant system for stable suspension of multiwalled carbon nanotubes (2010, neutral): “peaks and tangential-mode peaks [23].”
• Evaluating the characteristics of multiwall carbon nanotubes (2011, methodology): “For Raman scattering, MWCNTs can be said to be an ensemble of carbon nanotubes with diameters ranging from small to very large [35].”
• Carbon nanotubes, science and technology part (I) structure, synthesis and characterisation (2012, background): “However, for metallic tubes, the profile of the lower frequency component x G is broad, asymmetric and can be described by a Breit-Wigner-Fano (BWF) line shape Jorio et al., 2003; Colomer et al., 2001; Dresselhaus et al., 2002.”
• Raman spectroscopy of carbon nanotubes (2005, methodology): “This 2D phonon DOS can be recovered by summing the 1D phonon density of states for many SWNTs [1,13].”
• All-solid-state flexible micro-supercapacitor arrays with patterned graphene/MWNT electrodes (2014, background): “Junyeong Yun a, Daeil Kim a, Geumbee Lee b, Jeong Sook Ha a,b,* a Department of Chemical and Biological Engineering, Korea University, 5-1 Anam-dong, Seoul 131-701, Republic of Korea b KU-KIST Graduate School of Converging Science and Technology, 5-1 Anam-dong, Seoul 131-701, Republic of Korea A R T”
• Free-standing single-walled carbon nanotube/SnO2 anode paper for flexible lithium-ion batteries (2012, background): “In the first group, at low wave numbers between 150 and 300 cm, one finds the bands associated with radial breathing vibration modes (RBMs), whose peak positions are related to the tube diameter (d) through a relationship of the type vRBM (cm) = A/d (nm) + B, where A and B are constants that are det”
• 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]”