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Effect of buffer layer coupling on the lattice parameter of epitaxial graphene on SiC(0001)

T. Schumann, M. Dubslaff, M. H. Oliveira, Jr., M. Hanke, J. M. J. Lopes, and H. Riechert
Phys. Rev. B 90, 041403(R) – Published 8 July 2014
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Abstract

Grazing-incidence x-ray diffraction (GID) was employed to probe the structure of atomically thin carbon layers on SiC(0001): a so-called buffer layer (BL) with a 6(3×3)R30 periodicity, a monolayer graphene (MLG) on top of the BL, and a bilayer graphene (BLG). The GID analysis was complemented by Raman spectroscopy. The lattice parameter of each layer was measured with high precision by GID. The BL possesses a different lattice parameter and corrugation when it is uncovered or beneath MLG. Our results demonstrate that the interfacial BL is mainly responsible for the strain in MLG. By promoting its decoupling from the substrate via intercalation, it turns into graphene, leading to a simultaneous relaxation of the MLG and formation of a quasi-free-standing BLG.

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  • Received 13 May 2014
  • Revised 18 June 2014

DOI:https://doi.org/10.1103/PhysRevB.90.041403

©2014 American Physical Society

Authors & Affiliations

T. Schumann, M. Dubslaff, M. H. Oliveira, Jr.*, M. Hanke, J. M. J. Lopes, and H. Riechert

  • Paul-Drude-Institut für Festkörperelektronik, Hausvogteiplatz 5–7, 10117 Berlin, Germany

  • *Present address: Departamento de Física, ICEx, Universidade Federal de Minas Gerais-UFMG, C.P. 702, 31270-901, Belo Horizonte, MG, Brazil.
  • Corresponding author: lopes@pdi-berlin.de

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Issue

Vol. 90, Iss. 4 — 15 July 2014

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Images

  • Figure 1
    Figure 1

    Schematic structures (side view) of the samples investigated in the present study: (a) bare BL; (b) monolayer graphene on top of the BL; (c) bilayer graphene on top of an oxidized SiC surface (obtained by oxygen intercalation).

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  • Figure 2
    Figure 2

    Raman spectra of the three samples investigated in the present study: (a) bare BL; (b) monolayer graphene on top of the BL; (c) bilayer graphene on top of an oxidized SiC surface (obtained by oxygen intercalation upon air annealing).

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  • Figure 3
    Figure 3

    Reciprocal space map of monolayer graphene/BL on SiC(0001). The axes are scaled with the reciprocal lattice units (rlu) of SiC; qa and qr mark the radial and angular directions in the RSM.

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  • Figure 4
    Figure 4

    Line scans through the G(112¯0) reflection along qr, transformed to real space, performed for the bare BL, monolayer graphene/BL, and bilayer graphene samples. The dotted line indicates the value for the lattice parameter of graphite [31]. The x axis is scaled to the lattice parameter of graphene.

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