Raman spectroscopy of graphene and graphite: Disorder, electron phonon coupling, doping and nonadiabatic effects
By Andrea C. Ferrari. 2007
7,276 citations recorded by the source corpus.
Subfields: Materials Chemistry
View Paper: https://www.semanticscholar.org/paper/04e7b197209d40c5479400fc5a3c7332ec2ef605
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In Materials Chemistry
- A. Jorio
- K. Novoselov
- Zhenhua Ni
- Andrea C. Ferrari
- Mildred S. Dresselhaus
- T. Yu
- Zexiang Shen
- Luiz Gustavo Cançado
Citations in the corpus
- Vibrational properties of silicene and germanene (2012, methodology): “This discontinuity is reminiscent of the Kohn anomaly at K-point of graphene, which was identified as the physical origin of the linearly dispersive behavior of the phonon branch, in agreement with the experimental observation of the D peak dispersion with respect to the excitation energy [16].”
- Large-scale growth and characterizations of nitrogen-doped monolayer graphene sheets. (2011, background): “The G band shows a blue-shift compared to that from pristine monolayer graphene,(17) which is a sign of atomic insertions.(18) 20 The D band is accompanied by a D* band at∼1624 cm (1), Figure 2.”
- Simple procedure for an estimation of the coal rank using micro-Raman spectroscopy (2014, background): “Even though the area ratio of the D-band/G-band is the most common parameter illustrating the structural order of coal an carbonaceous material (Ferrari, 2007; Pusz et al., 2014; Tuinstra and Koenig, 1970), the intensities of the D- and Gbands (as well their ratio) will be strongly dependent on the ”
- Electronic transport in two-dimensional graphene (2010, background): “…achievement of Novoselov et al. (2004) in producing 2D graphene in the laboratory is not just fabricating (Novoselov et al., 2005b) and identifying (Ferrari, 2007; Ferrari et al., 2006) stable monolayers of graphene flakes on substrates, but also establishing its transport properties by gating the…”
- Production, properties and potential of graphene (2010, background): “[34] Raman spectra of carbon materials show similar features in the 800-2000 cm region, which is also of interest for graphene.[35-37] The G peak at around 1560 cm corresponds to the E2g phonon at the centre of the Brillouin zone.”