1993
DOI: 10.1016/0008-6223(93)90091-n
|View full text |Cite
|
Sign up to set email alerts
|

Raman spectroscopic characterization of graphites: A re-evaluation of spectra/ structure correlation

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

4
69
0
2

Year Published

1996
1996
2018
2018

Publication Types

Select...
6
2

Relationship

0
8

Authors

Journals

citations
Cited by 174 publications
(75 citation statements)
references
References 16 publications
4
69
0
2
Order By: Relevance
“…Raman spectroscopy is a useful characterization technique for carbon materials [37][38][39]. The first-order Raman spectrum of a single crystal of graphite exhibits a sharp peak at 1,582 cm -1 , which corresponds to the E 2g vibration mode (C-C vibration in the aromatic layers), is often referred as the G peak.…”
Section: Raman Spectroscopymentioning
confidence: 99%
“…Raman spectroscopy is a useful characterization technique for carbon materials [37][38][39]. The first-order Raman spectrum of a single crystal of graphite exhibits a sharp peak at 1,582 cm -1 , which corresponds to the E 2g vibration mode (C-C vibration in the aromatic layers), is often referred as the G peak.…”
Section: Raman Spectroscopymentioning
confidence: 99%
“…However, such a relation has been shown to yield an underestimate in L a for the case of nuclear-grade graphite. 16 This analysis was not applied to PPP-700, since the peaks observed in the Raman spectrum for this sample are influenced by the characteristics of the precursor more than by those of a typical graphitic material. In fact, a more careful study reveals that much of the peak intensities observed for PPP-700 arises from several A g modes of a highly disordered PPP molecular crystal.…”
Section: A 44åmentioning
confidence: 99%
“…4) proved to be very similar to graphite as regards to band positions (G*, D1) and eventually showed a lower fluorescence background when single particles were measured, instead [49] to 1620 [44] D1 D A 1g [40,53,56] ; edge effects as oxides or C¼C bonds [37,51] ; in plane defects and heteroatoms [43,45,54,64] ; sp 3 -sp 2 carbon bonds [8] ; volatile compounds, polyenes and ions [33] From 1301 to 1317 (for a NIR/IR excitation [47,51,58] ) to 1390 [49] D2 D′, G2 E′ 2g or E 2g or oxidized sp 2 carbons [37] ; non sandwiched graphene layers [51] ; defects as imperfect graphite or disordered E 2g [33,45,53,64] ; splitting of degenerated E 2g [41] ; E 1u [56] From 1599 [51] to 1635 [15,16,33,37,38,43,45,50,[53][54][55][56][64][65][66][67][68][69] …”
mentioning
confidence: 99%
“…[42] This band is also absent in highly ordered graphites. [43,45] The D1 band position is found to cover the whole range 1240 to 1400 cm À1 [46][47][48][49][50] and it shifts with the used laser wavelength. [45,49,51] Its intensity depends on the carbon type, [37] on the amount of disorder, [40] on the orientation of the crystal with respect to the laser [52] and on the measurement conditions.…”
mentioning
confidence: 99%