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Raman spectroscopy has been accepted to be a powerful and nondestructive tool to characterize the quality of graphitic materials.
This ID/IG ratio has been known to be inversely proportional to the grain size and provides a good estimation for the quality of graphitic materials [14].
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However, when used with certain types of graphitic materials, exfoliation occurs.
Finally, Figure 4F depicts the images of both SGS deformation and internalization of large pieces of graphitic materials.
In this research, different layers of graphitic materials were produced on the SS mesh via CVD technique.
The characteristic D line at 1360 cm-1 in the Raman spectra is a fingerprint of defects/disorder in the crystalline lattice of graphitic materials.
The degree of graphitization, defects and edge sites can be found by analyzing the relative intensities of these two lines depend on the type of graphitic materials [75].
The spectrum of graphitic materials and PANI/composites in Fig. 4 shows that PANI is dominant in all composites with various ratios.
In these production methods, the key challenge involves the exfoliation of graphitic materials in a liquid that can disperse graphene sheets in a stable way.
Graphene, a monolayer of carbon atoms which has a tight packing of honeycomb lattice and serves as the basic building block of graphitic materials, has recently become one of the most appealing stars in material science [1].
(30) The main features of graphitic materials in the Raman spectra were called G (∼1560 cm−1, E 2g mode, sp) and D (∼1360 cm−1, A1g mode, sp) bands for visible excitation, while the a-C band (T band) appears at ∼1060 cm−1 seen in UV excitation.
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