Quantifying defects in graphene via Raman spectroscopy at different excitation energies
L. G. Can\c{c}ado, A. Jorio, E. H. Martins Ferreira, F. Stavale, C. A., Achete, R. B. Capaz, M. V. O. Moutinho, A. Lombardo, T. Kulmala, and A. C., Ferrari

TL;DR
This study investigates how Raman spectroscopy can quantify defects in graphene at various excitation energies, providing a universal equation to determine defect density and resolving ambiguities using G peak analysis.
Contribution
It introduces a simple, energy-independent method to quantify defect density in graphene via Raman spectroscopy, accounting for excitation energy effects.
Findings
The D/G peak ratio depends strongly on excitation energy.
Maximum D/G ratio occurs at an inter-defect distance of ~3nm.
G peak analysis resolves ambiguity in defect density estimation.
Abstract
We present a Raman study of Ar(+)-bombarded graphene samples with increasing ion doses. This allows us to have a controlled, increasing, amount of defects. We find that the ratio between the D and G peak intensities for a given defect density strongly depends on the laser excitation energy. We quantify this effect and present a simple equation for the determination of the point defect density in graphene via Raman spectroscopy for any visible excitation energy. We note that, for all excitations, the D to G intensity ratio reaches a maximum for an inter-defect distance ~3nm. Thus, a given ratio could correspond to two different defect densities, above or below the maximum. The analysis of the G peak width and its dispersion with excitation energy solves this ambiguity.
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