Carbon nanomaterials such as graphene, graphite, and carbon nanotubes each have unique physical and thermal properties that make them important in industries as varied as battery manufacturing, construction, and sports equipment. The necessity for simple, safe, and robust characterization of these materials grows as they are more widely used in manufacturing settings.

Raman spectroscopy is a valuable tool for the characterization of carbon nanomaterials due to its selectivity, speed, and ability to measure samples nondestructively. Carbon materials typically exhibit simple Raman spectra, but they contain a wealth of information about internal microcrystalline structures in peak position, shape, and relative intensity.

Raman spectra of graphene-based materials, like those in Figure 1, are characterized by three major peaks: the G-band, the D-band, and the 2D-band.

The G-band appears near 1580 cm^-1 and represents the in-plane bending motion of doubly bonded carbon atoms. In high-quality graphene, the G-band is very sharp, indicating a high degree of crystallinity. The position of the G-band is sensitive to the number of graphene layers but is independent of laser excitation.

The D-band indicates disorder within a graphene sample. This band arises from a ring breathing mode for doubly bonded carbon atoms. In pristine graphene, the D-band is not visible. The D-band is observed when there is a defect in the graphene, or the mode is close to an edge. The D-band exhibits dispersive behavior, meaning that it is sensitive to the laser excitation wavelength used in the experiment.

The 2D-band is an overtone of the D-band, and the peak shape of the 2D-band can be used to determine layer thickness. Like the D-band, the 2D-band is dispersive and will change slightly with laser excitation.

An i-Raman® Prime 532H system was used for all measurements of graphene-based materials. The system has a 532 nm laser, which is the laser wavelength commonly chosen for Raman measurement of carbon. The i-Raman Prime is a low-noise, high-throughput, fully integrated Raman system with an embedded tablet computer.

A probe holder (BAC150B) was used for all measurements to support the fiber optic probe. An enclosure system (BAC152C) is available to achieve class 1 laser safety for a manufacturing floor. Typical laser power used is ~34 mW and acquisition times range from 30–90 s.

Determination of I_D/I_G

Guidelines for calculating I_D/I_G are documented in ASTM E3220 Standard Guide for Characterization of Graphene Flakes [2]. Spectra undergo baseline correction prior to peak intensity determination. For the spectra in Figure 3, a baseline removal algorithm was applied to data in the BWSpec software. The sharp peaks at ~1550 cm^-1 and ~2300 cm^-1 are attributed to atmospheric oxygen and nitrogen, respectively.

After baseline removal, peak intensities of spectral D- and G-bands are measured and I_D/I_G can be calculated. The software can be configured to automatically report I_D, I_G, and derived I_D/I_G from a collected spectrum. The results can be easily exported to a report. Table 2 shows the table that is generated in the software.

In Figure 3, nanofiber spectra are characterized by asymmetry in the G-bands. The I_D/I_G of spectrum (a) is particularly high, indicating that there is a high degree of structural disorder within that nanofiber sample.

The spectra from the carbon black samples (c–f) are categorized by broad D-bands and G-bands, indicating very low crystallinity within the samples. Measured I_D/I_G for the carbon black samples are all above 0.5, indicating structural disorder within the sample. I_D/I_G can be used as a quick offline or atline quality control test of manufactured graphene, graphite, carbon nanotubes, and carbon black powder.