Abstract

Raman spectroscopy is a technique widely used to detect defects in semiconductors because it provides information of structural or chemical defects produced in its structure. In the case of graphene monolayer, the Raman spectrum presents two bands centered at 1582 cm−1 (G band) and 2700 cm−1 (2D band). However, when the periodic lattice of graphene is broken by different types of defects, new bands appear. This is the situation for the Raman spectrum of graphene oxide. It is well established that the existence of these bands, the position and the intensity or width of peaks can provide information about the origin of defects. However, in the case of the graphene oxide spectrum, we can find in the literature several discrepant results, probably due to differences in chemical composition and the type of defects of the graphene oxide used in these studies. Besides, theoretical calculations proved that the shape of bands, intensity and width, and the position of graphene oxide Raman spectrum depend on the atomic configuration. In the current work, we will summarize our current understanding of the effect of the chemical composition on the Raman spectrum of graphene oxide. Finally, we apply all this information to analyze the evolution of the structure of graphene oxide during the thermal annealing of the heterostructures formed by graphene oxide sandwiches in a hexagonal boron nitride.

Highlights

  • Graphene oxide (GO) is a material derivate of graphene, which is produced by the oxidation of different types of graphite or carbon nanofibers

  • This paper summarized the reported Raman data of graphene oxides of different chemical compositions and structural defects

  • The results allowed us to obtain different correlations between the intensity, the position, and the width of the Raman spectrum and the crystallinity, oxidation degree, and structural defects of GO. We used these correlations to study the structural changes produced by thermal annealing of GO sandwiches between hexagonal boron nitride flakes

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Summary

Introduction

Graphene oxide (GO) is a material derivate of graphene, which is produced by the oxidation of different types of graphite or carbon nanofibers. From the structural point of view, it has a similar hexagonal carbon network to graphene; it contains different types of oxygen functional groups. The O-functionalization and the existence of structural defects on the basal plane due to the strong oxidation process remarkably reduce the excellent optoelectronic properties of graphene. Thermal annealing at high temperature (>750 ◦ C) significantly increases the C/O atomic ratio. It is necessary as an exhaustive control of the heat rate, because, if the temperature quickly increases, vacancies and other structural defects on the network have been observed [13]. The properties of GO can be modulated by introducing different functional groups and structural defects. This spectrum consists of two peaks centered at 1582 cm−1 (G band) and 2700 cm−1

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