Abstract

Studies of the effects induced on the electron band structure after Na deposition, and subsequent heating, on a C-face 2 MLs graphene sample are reported. Na deposition shifts the Dirac point downwards from the Fermi level by about 0.5 eV due to electron doping. After heating at temperatures from around 120℃ to 300℃,thep-band appears considerably broadened. Collected Si 2p and Na 2p spectra then indicate Na intercalation in between the graphene layers and at the graphene SiC interface. The broadening is therefore interpreted to arise from the presence of two slightly shifted, but not clearly resolved,p-bands. Constant energy photoelectron distribution patterns, E(kx,ky);s, extracted from the clean 2MLs graphene C-face sample look very similar to earlier calculated distribution patterns for monolayer, but not Bernal stacked bilayer, graphene. After Na deposition the patterns extracted at energies below the Dirac point appear very similar so the doping had no pronounced effect on the shape or intensity distribution. At energies above the Dirac point the extracted angular distribution patterns show the flipped, “mirrored”, intensity distribution predicted for monolayer graphene at these energies. An additional weaker outer band is also discernable at energies above the Dirac point, which presumably is induced by the deposited Na.

Highlights

  • Graphene grown epitaxially on the wide band semiconductor SiC is considered a most promising platform [1] for future carbon-based electronic devices

  • Constant energy photoelectron distribution patterns, E; s, extracted from the clean 2 MLs graphene C-face sample look very similar to earlier calculated distribution patterns for monolayer, but not Bernal stacked bi-layer, graphene

  • After Na deposition the patterns extracted at energies below the Dirac point appear very similar so the doping had no pronounced effect on the shape or intensity distribution

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Summary

Introduction

Graphene grown epitaxially on the wide band semiconductor SiC is considered a most promising platform [1] for future carbon-based electronic devices. Studies [6,7] of the electron band structure of graphene grown on Si-face SiC show that the number of -bands corresponds directly to the number of graphene layers. One -band ( -cone) with the Dirac point located close to the Fermi level has in general been observed [12,13,14] even for multilayer graphene samples. In this study the effects induced in the electron band structure of C-face graphene are investigated after depositing similar amounts of Na and after heating at similar temperatures as earlier done [3,5] for Si-face graphene samples. The idea was to see if similar effects could be induced on C-face graphene, that the Dirac point would shift downwards by one eV after deposition and if more than one -band could be observed after Na deposition and heating. Since Na do intercalate Si-face graphene we assumed that it would intercalate C-face graphene that is known to form in smaller domains/grains and have a higher density of defects on the surface

Experimental
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Summary and Conclusions
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