Nanoscale structural characterization of epitaxial graphene grown on off-axis 4H-SiC (0001)
© Vecchio et al; licensee Springer. 2011
Received: 3 November 2010
Accepted: 29 March 2011
Published: 29 March 2011
In this work, we present a nanometer resolution structural characterization of epitaxial graphene (EG) layers grown on 4H-SiC (0001) 8° off-axis, by annealing in inert gas ambient (Ar) in a wide temperature range (T gr from 1600 to 2000°C). For all the considered growth temperatures, few layers of graphene (FLG) conformally covering the 100 to 200-nm wide terraces of the SiC surface have been observed by high-resolution cross-sectional transmission electron microscopy (HR-XTEM). Tapping mode atomic force microscopy (t-AFM) showed the formation of wrinkles with approx. 1 to 2 nm height and 10 to 20 nm width in the FLG film, as a result of the release of the compressive strain, which builds up in FLG during the sample cooling due to the thermal expansion coefficients mismatch between graphene and SiC. While for EG grown on on-axis 4H-SiC an isotropic mesh-like network of wrinkles interconnected into nodes is commonly reported, in the present case of a vicinal SiC surface, wrinkles are preferentially oriented in the direction perpendicular to the step edges of the SiC terraces. For each T gr, the number of graphene layers was determined on very small sample areas by HR-XTEM and, with high statistics and on several sample positions, by measuring the depth of selectively etched trenches in FLG by t-AFM. Both the density of wrinkles and the number of graphene layers are found to increase almost linearly as a function of the growth temperature in the considered temperature range.
Graphene has attracted the interest of the scientific community due to its excellent electronic transport properties [1, 2], which make it a promising material for ultra-fast electronics operating in the 100 GHz to THz frequencies . Graphene was first obtained by mechanical exfoliation of highly oriented pyrolithic graphite (HOPG) . This is still the method of choice for basic studies on this material, because it produces high-crystalline quality graphene samples, which can be deposited on several substrates [4, 5]. However, the size of these flakes and the control of location on the substrate are not adequate for development of integrated circuit technologies. One major challenge to realize graphene electronics is to be able to produce large area and laterally uniform films. To date, the main routes toward large area graphene production include chemical vapor deposition (CVD) on metals , and controlled graphitization of hexagonal SiC by high-temperature thermal processes .
The latter method is the strongest candidate for graphene based electronics, owing to the fact that few layers of graphene (FLG) can be grown on a semiconductor substrate without any need to transfer (as is the case with CVD graphene on metal substrates). Graphene such produced is known as epitaxial graphene (EG). Graphene growth during annealing of SiC relies on the interplay of two different mechanisms: (i) the preferential Si sublimation from SiC surface, which leaves an excess of C atoms in the near surface region, and (ii) the diffusion of these C atoms on the SiC surface and their reorganization in the two-dimensional graphene lattice structure. Both mechanisms depend in a complex way both on the annealing conditions (temperature T gr, ramp rate, pressure in the chamber) and on the initial surface conditions of SiC wafers, e.g., the termination (Si- or C-face), the miscut angle, the defectivity. It has been shown that the rate of Si evaporation can be strongly reduced by performing the annealing in inert gas ambient at atmospheric pressure instead than in vacuum [8, 9]. This results in the possibility to raise the growth temperature, from typical values of T gr ~1300°C in vacuum to T gr > 1600°C at atmospheric pressure . This has, in turns, beneficial effects on the crystalline quality of the EG layers, since at higher temperature, a higher diffusivity of the C atoms on the surface is achieved. It has been also observed that graphene growth starts from the kinks of terraces on the SiC surface or from defects (e.g., pits or threading dislocations) . This means that, for fixed annealing conditions, a higher growth rate is expected on vicinal, i.e., off-axis, SiC surfaces than on on-axis ones, because the spacing between terraces kinks is reduced. Most of the studies on EG growth reported in the literature were carried out on on-axis hexagonal SiC substrates. However, off-axis 4H-SiC (0001) substrates with lowly doped epilayers are the standard platform for SiC technology. Hence, a detailed investigation on graphene growth on such substrates is mandatory, in the perspective of integrating future graphene electronics with current SiC technology.
In this work, we present a structural characterization of EG growth on the Si face of 8° off-axis 4H-SiC  by annealing in inert gas (Ar) ambient in a wide range of temperatures (T gr from 1600 to 2000°C). The modifications in the surface morphology after thermal treatments at the different temperatures were studied by tapping mode atomic force microscopy (t-AFM), showing the increase in the density of peculiar corrugations (wrinkles) in the EG multilayers with the growth temperature. High-resolution cross-sectional transmission electron microscopy (HRXTEM) was used to determine the number of graphene layers on very small sample areas. An alternative method to estimate the EG thickness on larger areas, based on etching out trenches selectively in graphitized SiC and measurements of the depth of those trenches by AFM, is also presented. The accuracy of this method is discussed.
Graphene growth was carried out in argon (Ar) ambient in a commercial furnace by Centrotherm Thermal Solutions GmbH + Co. KG, Blaubeuren, Germany at temperatures T gr from 1600 to 1700°C, or in an inductively heated reactor at T gr = 2000°C. The substrates used for graphene growth were lowly doped (approx. 1014 cm-3) epitaxially grown SiC layers on top of highly doped, 8° off-axis 4H-SiC (0001).
t-AFM measurements were carried out with Veeco DI3100 atomic force microscope fitted with Nanoscope V controller. Commercial silicon probes with spring constant k = 20 to 80 N/m, oscillation frequency 332 to 375 kHz in high-amplitude mode were employed.
Cross-sectional observations of the few layers of graphene grown on SiC were carried out using a JEOL JEM 2010F transmission electron microscope with a Schottky field emission gun operating at an acceleration voltage of 200 kV. Thin specimens for TEM observation were prepared by Ar-ion thinning by the following procedure: the graphene-on-SiC samples were mechanically ground to 70 μm thick, and the center of the sample was thinned by dimple grinding, followed by Ar-ion beam thinning under a low angle of 8° at 5 kV.
HRXTEM images allow an extremely precise determination of the number of grown layers, but on very small areas. An alternative method to determine the thickness of the grown FLG film on larger areas has been also developed. Stripes were patterned onto graphitized SiC substrates by optical lithography. Graphene was then selectively removed from these stripes with an O2 plasma (25 sccm) treatment for 16 min in an Roth & Rau Microsys 400 ICP-RIE (inductively coupled plasma) equipment. The step height between etched and not etched regions was determined by t-AFM. Before each t-AFM map, we acquired amplitude-distance curves both on not-etched and etched regions and the amplitude setpoint as well as the free amplitude were chosen accordingly, in order to operate in the repulsive interaction regime  on both surfaces.
The etch rates of graphene and bare SiC were calibrated independently. To this aim, graphene flakes were exfoliated from HOPG on SiC and their thickness was measured after different etching times by AFM. A patterned virgin SiC sample was etched under identical conditions and the etched depth was also measured by AFM. For the used plasma conditions, the etch rate of graphene is much higher than that of bare SiC.
Results and discussion
A root mean square (RMS) roughness of 0.2 nm is obtained from this surface analysis.
From the linescan in the direction parallel to the steps (d), it can be observed that the features in the morphology map are some peculiar corrugations with 1 to 2 nm typical height. These features appear on the phase linescan as a peak surrounded by two valleys. It is worth noting that these peculiar corrugations run preferentially in direction orthogonal to the step edges of the substrate.
In order to get further insight on the structural properties of the graphene films grown at the different temperature and to clarify the nature of these peculiar corrugations, HRXTEM analyses were carried out.
From Figure 4(b), the structure of one of the peculiar corrugations running orthogonal to the steps is reported. This cross sectional image unambiguously demonstrate that those features are wrinkles in the multilayer graphene film.
These peculiar defects have been observed also by other authors in the case of few layers of graphene grown on the C face  or on the Si face  of hexagonal SiC, on-axis. However, in that case, wrinkles do not exhibit any preferential orientation with respect to the steps, but form an isotropic mesh-like network on the surface, where wrinkles are interconnected into nodes (typically three wrinkles merge on a node and the angles subtended by the wrinkles are approx. 60 or 120°C ). The formation of that mesh-like network of wrinkles was attributed to the release of the compressive strain, which builds up in FLG during the sample cooling due to mismatch between the thermal expansion coefficients of graphene and the SiC substrate [13, 15]. In the present case of FLG grown on the Si face of off-axis 4H-SiC, a preferential orientation of the wrinkles orthogonal to the steps is observed. This peculiar effect suggests that compressive strain in FLG is released not only by the formation of parallel wrinkles inside each terrace, but also in an efficient way at step edges. This effect deserves further investigations.
Few-layers of graphene grown on 4H-SiC (0001) 8° off-axis, by annealing in inert gas ambient (Ar) in a wide temperature range (from 1600 to 2000°C) have been structurally characterized by atomic force microscopy and HR-XTEM. For all the considered growth temperatures, FLG conformally covering the 100 to 200-nm wide terraces of the SiC surface have been observed. The formation of wrinkles (approx. 1 to 2 nm high and 10 to 20 nm wide) preferentially oriented in the direction perpendicular to the step edges of the SiC terraces has been observed in the FLG film, as a result of the release of the compressive strain accumulated in FLG during the sample cooling due to the thermal expansion coefficients mismatch between graphene and SiC. This parallel orientation of wrinkles is peculiar of EG grown a vicinal SiC surface, whereas for EG grown on on-axis 4H-SiC an isotropic mesh-like network of wrinkles interconnected into nodes is commonly reported. The observed phenomenon deserves further investigations. Both the density of wrinkles and the number of graphene layers are found to increase almost linearly as a function of the growth temperature in the considered temperature range.
chemical vapor deposition
few layers of graphene
high-resolution cross-sectional transmission electron microscopy
highly oriented pyrolithic graphite
root mean square
tapping mode atomic force microscopy
The authors acknowledge S. Di Franco from CNR-IMM, Catania for his skillful technical assistance. Epitaxial Technology Center (ETC) is acknowledged for providing SiC substrates. This publication has been supported, in part, by the European Science Foundation (ESF) under the EUROCORE program EuroGRAPHENE, within GRAPHIC-RF coordinated project.
- Novoselov KS, Geim AK, Morozov SV, Jiang D, Zhang Y, Dubonos SV, Grigorieva IV, Firsov AA: Electric Field Effect in Atomically Thin Carbon Films. Science 2004, 306: 666–669. 10.1126/science.1102896View ArticleGoogle Scholar
- Zhang Y, Tan YW, Stormer HL, Kim P: Experimental observation of the quantum Hall effect and Berry's phase in graphene. Nature 2005, 438: 201–204. 10.1038/nature04235View ArticleGoogle Scholar
- Chen JH, Jang C, Xiao S, Ishigami M, Fuhrer MS: Intrinsic and extrinsic performance limits of graphene devices on SiO 2, . Nat Nanotechnol 2008, 3: 206–209. 10.1038/nnano.2008.58View ArticleGoogle Scholar
- Sonde S, Giannazzo F, Vecchio C, Yakimova R, Rimini E, Raineri V: Role of graphene/substrate interface on the local transport properties of the two-dimensional electron gas. Appl Phys Lett 2010, 97: 132101. 10.1063/1.3489942View ArticleGoogle Scholar
- Giannazzo F, Sonde S, Raineri V, Rimini E: Screening Length and Quantum Capacitance in Graphene by Scanning Probe Microscopy. Nano Lett 2009, 9: 23. 10.1021/nl801823nView ArticleGoogle Scholar
- Kim KS, Zhao Y, Jang H, Lee SY, Kim JM, Kim KS, Ahn JH, Kim P, Choi JY, Hong BH: Large-scale pattern growth of graphene films for stretchable transparent electrodes. Nature 2009, 457: 706. 10.1038/nature07719View ArticleGoogle Scholar
- Berger C, Song Z, Li X, Wu X, Brown N, Naud C, Mayou D, Li T, Hass J, Marchenkov AN, Conrad EH, First PN, de Heer WA: Electronic confinement and coherence in patterned epitaxial graphene. Science 2006, 312: 1191–1195. 10.1126/science.1125925View ArticleGoogle Scholar
- Emtsev KV, Bostwick A, Horn K, Jobst J, Kellogg GL, Ley L, McChesney JL, Ohta T, Reshanov SA, Rohrl J, Rotenberg E, Schmid AK, Waldmann D, Weber HB, Seyller T: Towards wafer-size graphene layers by atmospheric pressure graphitization of silicon carbide. Nature Mater 2009, 8: 203. 10.1038/nmat2382View ArticleGoogle Scholar
- Virojanadara C, Syvajarvi M, Yakimova R, Johansson LI, Zakharov AA, Balasubramanian T: Homogeneous large-area graphene layer growth on 6 H -SiC(0001). Phys Rev B 2008, 78: 245403. 10.1103/PhysRevB.78.245403View ArticleGoogle Scholar
- Bolen ML, Harrison SE, Biedermann LB, Capano MA: Graphene formation mechanisms on 4H-SiC(0001). Phys Rev B 2009, 80: 115433. 10.1103/PhysRevB.80.115433View ArticleGoogle Scholar
- Sonde S, Giannazzo F, Raineri V, Yakimova R, Huntzinger JR, Tiberj A, Camassel J: Electrical properties of the graphene/4 H -SiC (0001) interface probed by scanning current spectroscopy. Phys Rev B 2009, 80: 241406(R). 10.1103/PhysRevB.80.241406View ArticleGoogle Scholar
- Nemes-Incze P, Osvath Z, Kamaras K, Biro LP: Anomalies in thickness measurements of graphene and few layer graphite crystals by tapping mode atomic force microscopy. Carbon 2008, 46: 1435. 10.1016/j.carbon.2008.06.022View ArticleGoogle Scholar
- Prakash G, Capano MA, Bolen ML, Zemlyanov D, Reifenberger RG: AFM study of ridges in few-layer epitaxial graphene grown on the carbon-face of 4H SiC(000–1). Carbon 2010, 48: 2383. 10.1016/j.carbon.2010.02.026View ArticleGoogle Scholar
- Sun GF, Jia JF, Xue QK, Li L: Atomic-scale imaging and manipulation of ridges on epitaxial graphene on 6H-SiC(0001). Nanotechnology 2009, 20: 355701. 10.1088/0957-4484/20/35/355701View ArticleGoogle Scholar
- Röhrl J, Hundhausen M, Emtsev KV, Seyller T, Graupner R, Ley L: Raman spectra of epitaxial graphene on SiC(0001). Appl Phys Lett 2008, 92: 201918.View ArticleGoogle Scholar
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