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Surface Chemistry Involved in Epitaxy of Graphene on 3C-SiC(111)/Si(111)
© The Author(s) 2010
Received: 25 June 2010
Accepted: 2 August 2010
Published: 14 August 2010
Surface chemistry involved in the epitaxy of graphene by sublimating Si atoms from the surface of epitaxial 3C-SiC(111) thin films on Si(111) has been studied. The change in the surface composition during graphene epitaxy is monitored by in situ temperature-programmed desorption spectroscopy using deuterium as a probe (D2-TPD) and complementarily by ex situ Raman and C1s core-level spectroscopies. The surface of the 3C-SiC(111)/Si(111) is Si-terminated before the graphitization, and it becomes C-terminated via the formation of C-rich (6√3 × 6√3)R30° reconstruction as the graphitization proceeds, in a similar manner as the epitaxy of graphene on Si-terminated 6H-SiC(0001) proceeds.
Graphene, a single layer of sp2-bonded carbon, has fabulous electronic, mechanical, and optical properties . Graphene is thus expected to be various kinds of applications. Owing to its industrial adaptability, epitaxial graphene (EG) formed by annealing of SiC bulk crystal is attracting recent attentions [2–4]. EG, however, face two challenges: the limited diameter of the substrate and the low cost-performance in the current price. To overcome these challenges, we have been investigating the use of SiC thin films on Si substrates, instead of SiC bulk crystals, in the formation of graphene. We have actually succeeded in fabricating a graphene on an epitaxial SiC thin film on Si substrate by sublimating silicon atoms from the surface of the epitaxial SiC thin film [5, 6]. This graphene-on-silicon (GOS) method has a potential of forming graphene films on large-scale Si wafers. GOS is therefore compatible with the silicon technology [5, 6].
The film quality of GOS, however, still remains as a challenge. This undoubtedly requires detailed understanding of the graphitization mechanism in GOS as a prerequisite. In the case of epitaxial graphene formation on Si-face 4H- or 6H-SiC(0001) substrates, several groups [2–4] have reported that graphene (1 × 1) is formed after the appearance of two SiC reconstructions: (√3 × √3)R30° and (6√3 × 6√3)R30° in this order. GOS process on Si(111) substrates follows this process . To go further into the clarification of the mechanism of graphitization, however, the surface chemical component for each reconstruction needs to be probed. Hirayama et al. conducted temperature-programmed desorption measurement on molecular hydrogen (H2-TPD) for each of the reconstructed surfaces of 6H-SiC(0001) . They concluded that the hydrogen adsorption site shifts from Si to C after graphitization, but detailed identification of the H2-TPD peaks has not been given yet. In this study, we have conducted TPD using molecular deuterium (D2-TPD) to investigate the surface chemistry involved in the GOS process on 3C-SiC(111)/Si(111). TPD serves as an in situ probe for the chemical component of the surface. C1s core-level and Raman spectroscopies have also been used as complementary means to support the understandings given by D2-TPD.
A p-type Si(111) wafer (0.400–0.600 Ω cm) was cut into pieces to form specimens sized with 7 × 40 mm2. The specimen, after degreased by ultrasonication in acetone and ethanol, was introduced into the UHV chamber (base pressure: ~10−10 torr) and flash-annealed at 1,473 K (Sample A). The epitaxial 3C-SiC thin films, ~100 nm in thickness, were grown by exposing the DC-heated Si substrate (1,323 K) to a CH3SiH3 (MMS) gas [5, 6]. The samples were then annealed either at 1,273 K for 10 s (Sample B), 1,423 K for 60 min (Sample C), or 1,523 K for 30 min (Sample D) [2, 3]. After annealing, each sample was exposed to a flux of atomic deuterium, made by cracking of D2 molecules (~10−4 Pa) by a hot tungsten filament (1,673 K). D2-TPD spectrum was then obtained by gradually increasing the sample temperature at a rate of 5 K/s. Raman and C1s core-level spectroscopies were also performed ex situ. The excitation energy in the Raman spectroscopy is 2.41 eV. The X-ray source for the C1s core-level spectroscopy is non-monochromatized Mg–Kα (1,253.6 eV).
Results and Discussion
The TPD spectrum of the graphene overlayer on 3C-SiC(111)/Si(111) (Sample D) drastically changes, as demonstrated in Fig. 1(d). Two distinct peaks around 1,100 K and 1,300 K are due to desorption of deuterium bonded with sp2-bonded carbon atoms in the graphene overlayer, while the peaks due to deuterium desorption from D-Si of the SiC thin film and Si substrate (<1,000 K) are not observed. The Raman spectrum of the graphene overlayer (Fig. 2(iii)) displays the G′ band, in addition to the G and the D bands. The presence of the G′ band indicates the well-ordered graphene overlayer because the appearance of G′ band is the consequence of the high degree of the crystallinity of the graphene layer . Further, the G′ band consists of multiple components, as can be seen from the line shape of the G′ band. This indicates that the graphene layers are Bernal stacked . This is supported by the C1s core-level spectrum (Fig. 3). In the spectrum, the peak due to sp2-bonded carbon atoms (~284.3 eV) is dominant, and the component due to the (6√3 × 6√3)R30°-reconstructed layer (~285.2 eV) is still observed. It can be thus concluded that the graphene overlayer grows on the (6√3 × 6√3)R30°-reconstructed layer as the epitaxy of graphene on 6H-SiC(0001). This can explain the disappearance of the peaks (D x -Si(C)) that is related with the (6√3 × 6√3)R30°-reconstructed layer in the TPD spectrum of sample D, because graphene overlayer blocks adsorption or desorption of deuterium onto the surface.
We have probed the epitaxial processes of graphene on 3C-SiC(111)/Si(111) in situ by D2-TPD spectroscopy, and complemental ex situ spectroscopies, such as Raman spectroscopy and C1s core-level spectroscopy. The results obtained in this study indicate that the epitaxy of graphene on 3C-SiC(111)/Si(111) proceeds in a similar manner to that on hexagonal SiC(0001) bulk crystals.
The work was supported by CREST, the Japan Science and Technology Agency (JST), Japan.
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- Geim AK: Science. 2009, 324: 1530. COI number [1:CAS:528:DC%2BD1MXnsFOrsLk%3D]; Bibcode number [2009Sci...324.1530G] 10.1126/science.1158877View ArticleGoogle Scholar
- Riedl C, Starke U, Bernhardt J, Franke M, Heinz K: Phys. Rev. B. 2007, 76: 245406. Bibcode number [2007PhRvB..76x5406R] Bibcode number [2007PhRvB..76x5406R] 10.1103/PhysRevB.76.245406View ArticleGoogle Scholar
- Rollings E, Gweon G-H, Zhou SY, Mun BS, McChesney JL, Hussain BS, Fedorov AV, First PN, de Heer WA, Lanzara A: J. Phys Chem Solids. 2006, 67: 2172–2177. COI number [1:CAS:528:DC%2BD28XptlSqu7w%3D]; Bibcode number [2006JPCS...67.2172R] 10.1016/j.jpcs.2006.05.010View ArticleGoogle Scholar
- Mallet P, Varchon F, Naud C, Magaud L, Berger C, Veuillen J-Y: Phys. Rev. B. 2007, 76: 041403. Bibcode number [2007PhRvB..76d1403M] Bibcode number [2007PhRvB..76d1403M] 10.1103/PhysRevB.76.041403View ArticleGoogle Scholar
- Miyamoto Y, Handa H, Saito E, Konno A, Suemitsu M, Fukidome H, Ito T, Yasui K, Nakazawa H, Endoh T: e-J. Surf. Sci Nanotech.. 2009, 7: 107–109. COI number [1:CAS:528:DC%2BD1MXislyjur8%3D] 10.1380/ejssnt.2009.107View ArticleGoogle Scholar
- Suemitsu Yu Miyamoto M, Handa Hiroyuki, Konno Atsushi: e-J. Surf. Sci. Nanotech. 2009, 7: 311–313. 10.1380/ejssnt.2009.311View ArticleGoogle Scholar
- Suemitsu M, Fukidome H: J. Phys. D., in press.Google Scholar
- Aoki Y, Hirayama H: Appl. Phys. Lett.. 2009, 95: 094103. Bibcode number [2009ApPhL..95i4103A] Bibcode number [2009ApPhL..95i4103A] 10.1063/1.3223598View ArticleGoogle Scholar
- Kim H, Taylor N, Spila T, Glass G, Park SY, Greene JE, Abelson JR: Surf. Sci.. 1997, 380: 496–500. 10.1016/S0039-6028(96)01587-7View ArticleGoogle Scholar
- Konno A, Senthil K, Murata T, Suemitsu M: Appl. Surf. Sci.. 2006, 252: 3692–3696. COI number [1:CAS:528:DC%2BD28Xhs1Gkt7g%3D]; Bibcode number [2006ApSS..252.3692K] 10.1016/j.apsusc.2005.05.052View ArticleGoogle Scholar
- Riedl C, Coletti C, Iwasaki T, Zakharov AA, Starke U: Phys. Rev. Lett.. 2009, 103: 246804. COI number [1:STN:280:DC%2BC3c3jslGktQ%3D%3D]; Bibcode number [2009PhRvL.103x6804R] 10.1103/PhysRevLett.103.246804View ArticleGoogle Scholar
- Virojanadara C, Zakharov AA, Yakimova R, Johanson LI: Surf. Sci.. 2007, 604: 4–7. 10.1016/j.susc.2009.11.011View ArticleGoogle Scholar
- Schenk A, Winter B, Biener J, Lutterioh C, Schubert UA, Küppers J: J. Appl. Phys.. 1995, 77: 6.Google Scholar
- Zhao X, Outlaw RA, Wang JJ, Zhu MY, Smith GD, Holloway BC: J. Chem. Phys.. 2006, 124: 194704. COI number [1:STN:280:DC%2BD28zgtlCgsg%3D%3D]; Bibcode number [2006JChPh.124s4704Z] 10.1063/1.2187969View ArticleGoogle Scholar
- Emtsev KV, Speck E, Seyller Th, Ley L: Phys. Rev. B.. 2008, 77: 155303. Bibcode number [2008PhRvB..77o5303E] Bibcode number [2008PhRvB..77o5303E] 10.1103/PhysRevB.77.155303View ArticleGoogle Scholar
- Pimenta MA, Dresselhaus G, Dresselhaus MS, Cançado LG, Jorio A, Saito R: Phys. Chem. Chem. Phys.. 2007, 9: 1276. COI number [1:CAS:528:DC%2BD2sXisFCntrc%3D] 10.1039/b613962kView ArticleGoogle Scholar