AVS 60th International Symposium and Exhibition
    Graphene and Other 2D Materials Focus Topic Tuesday Sessions
       Session GR+AS+NS+SP+SS-TuA

Paper GR+AS+NS+SP+SS-TuA9
Purity, Structure and Electronic Properties of Graphene Studied by Low Energy Ion Scattering

Tuesday, October 29, 2013, 4:40 pm, Room 104 B

Session: Characterization including Microscopy and Spectroscopy of 2D Materials
Presenter: T. Grehl, ION-TOF GmbH, Germany
Authors: S. Prusa, Brno University of Technology, Czech Republic
P. Prochazka, Brno University of Technology, Czech Republic
P. Babor, Brno University of Technology, Czech Republic
P. Bruener, ION-TOF GmbH, Germany
T. Grehl, ION-TOF GmbH, Germany
R. ter Veen, Tascon GmbH, Germany
H. Brongersma, ION-TOF GmbH, Tascon GmbH, Germany
Correspondent: Click to Email

Based on the unique electronic properties and high chemical stability of graphene, a number of exciting applications are generated. However, since graphene films are only one or a few atomic layers thick, chemical analysis is hampered by the much larger information depth of most techniques. This leaves a gap which can be filled by Low Energy Ion Scattering (LEIS). LEIS is known for its extreme surface sensitivity. It gives a quantitative analysis of the outer atomic layer of a surface as well as in-depth information [1]. It can thus be used to selectively analyze a graphene layer. In general [2], the atomic sensitivities are independent of the neighboring atoms (no matrix effects), so a quantitative elemental characterization is feasible. Since carbon is a common contamination in surface analysis, it is crucial to distinguish such contamination from the carbon in graphene.

In an earlier LEIS study [3] of carbon segregation in C-doped rhenium it was shown that by varying the temperature the carbon species can be altered reversibly into a carbidic or graphitic state. The graphitic layer was one or a few atoms thick (depending on the temperature). A strong matrix effect was observed in LEIS, which is believed to be typical for graphene. The sp-band of graphitic carbon is so wide that it extends to the He 1s level. This gives a strong quasi-resonance neutralization of the scattered He+ ions.

In the present study graphene layers were grown on copper foils and then transferred to an oxidized Si wafer [4]. The samples were analyzed with a dedicated high-sensitivity LEIS instrument. As reference for a carbon containing material without a wide conduction band, silicon rubber was chosen.

It was found that the neutralization of He+ by graphene is much stronger than by the rubber. For example, the neutralization of 1.5 keV He+ ions is almost 100x more effective for graphene.

It will be shown how it is possible to quantify the amount of carbon contamination (hydrocarbons, alcohols, etc.) on graphene using the differences in neutralization. Thus LEIS cannot only be used to verify the closure of the graphene layer, its thickness and purity, but also to check its (wide band) electronic structure.

[1] H.H. Brongersma, Low-Energy Ion Scattering, in: Characterization of Materials, J. Wiley & Sons (2012). DOI: 10.1002/0471266965.com144

[2] H.H. Brongersma, M. Draxler, M. de Ridder, P. Bauer, Surf. Sci. Repts 62 (2007) 63-109.

[3] L.C.A. van den Oetelaar, S.N. Mikhailov, H.H. Brongersma, Nucl. Instrum. Meth. B85 (1994) 420.

[4] Xuesong Li et al., Science 324, 1312 (2009). DOI: 10.1126/science.1171245