The seeded growth of graphene.

In this paper, we demonstrate the seeded growth of graphene under a plasma chemical vapor deposition condition. First, we fabricate graphene nanopowders (~5 nm) by ball-milling commercial multi-wall carbon nanotubes. The graphene nanoparticles were subsequently subject to a direct current plasma generated in a 100 Torr 10%CH4 - 90%H2 gas mixture. The plasma growth enlarged, over one hour, the nuclei to graphene sheets larger than one hundred nm(2) in area. Characterization by electron and X-ray diffraction, high-resolution transmission electron microscopy images provide evidence for the presence of monolayer graphene sheets.

Graphene layers, as a result of weak van der Waals attraction, cause the material to adopt a stacked multilayer configuration1 and make it difficult to deposit or fabricate a perfect 2-dimensional structure23. For example, graphene formed on a metal substrate by chemical vapour deposition (CVD) appears as single and multiple graphene layers456 which may be regarded as azimuthally aligned graphite rather than graphene. Furthermore, monolayer graphene (~0.4 nm in thickness) is very seldom produced even in the samples prepared by micromechanical cleavage278. The yield of graphene via a mass production chemical route910111213 may be also very low because the residues in the centrifuged supernantant liquid are only ~0.5% of the starting material9. The chemical approach to fabricating monolayer graphene has two fundamental problems. First, it is energetically difficult for molecules to intercalate the graphite layers. For example, intercalation of relatively small lithium atoms into graphite requires >0.5 eV/atom14. Secondly, isolated graphene planes may restack during further treatment in suspension. The relative effective area of graphene for van der Waals interactions is much larger, by approximately two orders of magnitude, than that of untreated single-wall carbon nanotubes (SWNTs) which exist as bundles15. Indeed, there have been no reports showing direct evidence of the presence of monolayer graphene powders, such as broadened 002 peaks in X-ray diffraction (XRD) patterns together with high-resolution transmission electron microscopy (HRTEM) images showing separated monolayer graphene although there are many reports9101112131617 of the large-scale production of graphene.

Recently we have shown that multi-wall carbon nanotubes (MWNTs) are composed of AA′ stacked graphene helices where width is of the order of a few nanometers18, unlike the conventional view of the structure of MWNTs: a tubule comprising concentrically nested graphene sheets19. This observation suggests that shortening helical graphitic materials, exhibiting a high aspect ratio (~1,000), may form nano-scale monolayer graphene. In this work, we fabricate graphene nanopowders (GNPs) with a size of ~5 nm by ball-milling commercial MWNTs, and demonstrate that the GNPs used as nuclei grow to monolayer graphene sheets under a plasma CVD condition.

Results

Figure 1 shows HRTEM images before (a) and after (b and c) mechanical milling of MWNTs for varying periods of time. The pristine tubules reveal the unique bamboo morphology1819 evident of our helical MWNTs18. With an hour of milling, the tubules were decomposed to graphitic nanoribbons whose thickness and width are ~5 nm, respectively (b). The graphitic nanoribbons were cleaved into graphene nanopowders (GNPs) of a few nm in length with another 1 hour milling (c), as shown in Fig. 1c′. GNPs are randomly oriented although stacked graphene fringes are partially observed. The variation of electron diffraction (ED) patterns (inset) is consistent with the dramatic change of the materials from tubular MWNTs (a) where the 002 spots appear as two spots, via stacked nanoribbons (b), to GNPs (c) where the 002 spots are transformed into a diffused ring. The ED pattern of the sample milled for 2 hours exhibited diffuse rings (Fig. 1c) providing evidence for the presence of graphene in the form of powders.

Figure 1

HRTEM images showing a mechanical conversion of MWNTs into GNPs.

(a), Pristine VCCVD-MWNT showing the graphene helices released from the walls. (b), Milled for 1 hour. (c), (c′), Milled for 2 hours.

XRD analysis of the samples provides more specific information as to the structural changes of the MWNTs following milling. The data showed that 002, 020, 004, and 200 peaks of orthorhombic AA′ graphene stacked MWNTs16 broadened with 2 hours milling, as shown in Fig. 2a and b, confirming the entire decomposition of the pristine material into GNPs. The full width at half maximum (FWHM) value of 002 peak increased from 2.2° (pristine MWNT) to 7.6° where the mean inter-planar spacing of 3.60 Å was determined (Fig. 2b). The purified GNPs (purified in alcohol solution: see Methods) evolved a saw-tooth like 002 peak, as shown in Fig. 2c. The mean inter-planar spacing and FWHM value of the unique 002 peak were measured to be 3.48 Å and 4.5°, respectively.

Figure 2

XRD patterns of the samples and schematic explaining the states of the samples with the processes.

(a), XRD pattern of pristine VCCVD-MWNTs where characteristic peaks are assigned to an orthorhombic AA′ crystal. (b), XRD pattern of as milled GNPs where 002 peak is broadened with milling for 2 hours. Blue arrows indicate signals of metal impurities originated from the steel balls. (c), XRD pattern of purified GNPs where 002 peak is evolved after purification. Ordered graphene layers (a′) are scattered by milling and exist disorderly with metal impurities (b′). During dry after purification graphene layers are packed by tension of alcohol (b″). The packing can be classified as either parallel or random packing (c′).

The GNPs grew to form graphene plates of hundred nm2 in area when the nanographene seeds were subject to a direct current plasma, as shown in the HRTEM image in Fig. 3. The characteristic hexagonal atomic lattices (Fig. 3b) and the corresponding unique FFT image yield an hexagonal array of spots (inset) and the edges of monolayer graphene5820 are clearly observable in the image. The prominent edge structures of graphene sheets are also observable in the conventional HRTEM (working at 200 kV) images as shown in Fig. 4a and b where bi- and trilayer graphene sheets (i.e., thin graphite) are also observable. The isolated graphene sheet (Fig. 4a) shows a faceted outline where the crystal edges subtended an angle of 120°. Graphene sheets with lateral dimensions of several tens nm2 exhibiting layer edges are evident in Fig. 4b which appear mostly to be curved and overlapped.

Figure 3

Schematic explaining the seeded growth of graphene and HRTEM images.

(a), Schematic explaining the seeded growth of graphene under a plasma condition. (b), Titan HRTEM (operating at 80 kV) image of a graphene sheet. The yellow line passing through the atomic lattices is a visual indication of the single crystal graphene sample. We attribute local mosaic lattices to overlaps of smaller graphene fragments. The inset is FFT diffraction pattern of the region indicated in (b). (c), Inverse FFT image taken from the region indicated in (b).

Figure 4

HRTEM images of the graphene samples.

Conventional HRTEM (operating at 200 kV) images showing graphene and bi- and trilayer graphene sheets (i.e., thin graphite). The schematic explains the faceted growth of the isolated graphene sheet. Overlapped graphene layers are also observable in (b). Black arrows indicate the intersections of graphene layers.

Figure 5 shows the Raman spectra of MWNTs, GNPs, and plasma treated GNR samples. The typical peaks of MWNTs broaden (D and G) or disappear (2D i.e., G′) in the spectrum of GNPs formed by two hours milling. Intense narrow peaks appear in the Raman spectrum of the graphene samples. The feature is different from those of monolayer graphene4521 as well as graphite21 since the relative intensity of the D peak is very strong.

Figure 5

Raman spectra of MWNTs, GNPs, and seeded grown graphene samples.

The typical peaks of MWNTs broaden (D and G) or disappear (2D) in the spectrum of GNPs formed by two hours milling. The Raman spectrum of the graphene samples reveals relatively intense narrow peaks.

Discussion

The broad 002 peak with the d-value of 3.60 Å of the milled samples (Fig. 2b) indicates that GNPs exist as randomly oriented (Fig. 2b′) because the inter-planar spacing is larger than those of crystalline graphite, namely, 3.35 Å for AB stacking, 3.44 Å for AA′ stacking and 3.53 Å for AA stacking1. The variation of the 002 peak following the purification treatment (Fig. 2b and c) can be explained in terms of stacking between GNPs. The stacking of randomly oriented GNPs (Fig. 2b′) may be due to the surface tension and capillary forces of residual alcohol (Fig. 2b″) or by van der Waals interaction (Fig. 2c′) when completely dry. The packing can be classified as either parallel or random packing according to the distribution of the azimuthal angle between the planes (Fig. 2c′). The former can be regarded as two-dimensionally disordered (turbostratic) structure where the crystallographic relationship22 between the graphene layers is absent. The two-dimensionally disordered structure includes locally AB, AA′, and AA (Fig. 1 of ref. 18) stacking and, thus, its mean interplanar spacing lies between 3.35 Å (smallest) for AB stacking and 3.53 Å (largest) for AA stacking1. This explains the measured inter-planar spacing of GNPs of ≈3.48 Å. The three-dimensionally disordered structure of the GNPs with a large distribution of the inter-planar spacings, explains the wide base of the 002 peak (Fig. 2c). The explanation for the unique variation of the XRD patterns before and after the solution treatment of GNPs is consistent with the structure of graphene and attraction between the GNPs.

The intersections (black arrows) in Fig. 4a and b of graphene layers indicate that thin graphite may be formed by joining preformed graphene sheets (i.e., independently nucleated) with van der Waals interaction during the CVD growth although we do not exclude the possibility that it was originated from stacked GNP nuclei. We attribute the unique Raman spectrum (strong D peak) of the plasma seeded grown graphene samples to the coexistence of “nano-sized” graphene and thin graphite. The large fraction of the edge structure can increase the relative intensity of the D peak which is related with defects within disordered graphene. The Raman data represent the average signal of numerous graphene and thin graphite nanosheets included within the Raman laser beam where the beam diameter is 1–2 μm (see Methods). The intensity ratio of 2D peak to G peak, I2D/IG, is about 0.62, and this value is similar to those for the graphene samples grown on Co or Ni (see Table 1 of Ref. 23). The relatively strong G and 2D (G′) peaks of the plasma treated GNP samples compared with those of GNPs as well as MWNTs demonstrates the outgrowth of well-crystallized graphene layers during the secondary growth from GNPs.

We propose a mechanism for the plasma growth of graphene via the lateral growth of the zigzag lines of graphene which subtend angles of 120° (see Fig. 4 of Ref. 24). The zigzag line, which is the closest-packed edge with higher surface energy than that of the armchair edge24, can form the template for further growth by the incorporation of carbon species from the plasma. The isolated and faceted graphene grain shown in Fig. 4a resulted from long range lateral growth of the zigzag edges of the graphene crystal.

The overlap of the graphene sheets shown in Fig. 4b could conceivably have occurred during TEM sampling, including a solution treatment where the samples are dispersed in alcohol and deposited on a TEM grid with the conditions of Fig. 2b″ and c′. We attribute the edges shown in Fig. 3b and 4b, unlike the case of the isolated graphene sheet (Fig. 4a), to distortion of the edge lines by stresses. With the evolution of the (002) XRD peak from solution treated GNPs (Fig. 2c), the appearance of overlapping graphene sheets (Fig. 4b) supports our view that it will be difficult to produce monolayer graphene via chemical routes.

The HRTEM images showing the edges of monolayer graphene (Fig. 3b and 4) provide unequivocal evidence of the presence of monolayer graphene. The data are to be compared with the previously reported low magnification TEM images1317252627 where atomic graphene layers cannot be confirmed, cross-sectional HRTEM images where graphene layers appear unclearly232829, and atomic resolution (in-plan) HTRTEM images showing hexagonal lattices6783031323334, which are obtainable from bi- or trilayer graphene (i.e., thin graphite)6833. ED patterns showing hexagonal symmetry131725272829303135 are also obtainable either from bilayer graphene (Fig. 5b of ref. 6) or single crystal graphite36.

In summary, the outgrowth of graphene from the GNP nuclei was achieved at a plasma CVD condition thus producing a new method of forming graphene sheets larger than one hundred nm2 in area. Characterization by electron and X-ray diffraction, high-resolution transmission electron microscopy provides direct evidence of the presence of pure monolayer graphene.

Methods

Synthesis of graphene

Commercial MWNTs (CM-95, 95 wt% purity, Hanwha nanotech), prepared by VCCVD technique, were used as a starting material for the fabrication of graphene nanopowders (GNPs) to be served as nuclei for the seeded plasma growth of graphene. Diameters and lengths of the MWNT samples were 10–20 nm and 3–20 μm respectively. 1 g of the samples was loaded into a steel jar (Φ 60 × 60 L) with twenty steel balls (each 2 g) and processed by a conventional (Spex) milling apparatus for 1 ~ 6 hours. For the novel CVD growth, the purified GNPs which were prepared on a molybdenum substrate were subjected to a direct current plasma generated at 100 Torr of a 10%CH4-90%H2 gas mixture for I hour. The temperature of the substrate was kept at 1,200°C.

Characterization of graphene

The milled samples, i.e., GNPs were confirmed by HRTEM observation as well as X-ray diffraction pattern analysis. The GNPs including metal particles originated from the steel balls were purified through a solution treatment where the samples are dispersed in ethyl alcohol with sonication and the metal impurities are removed by magnets. HRTEM observation for grown graphene sheets were performed by a JEM-2100F operating at 200 kV and a FEI Titan Cubed with aberration corrector and a monochrometer operating at 80 kV. Raman analysis was performed by a Renishaw In-Via Raman Microscope with laser excitation of 532 nm and spot size of 1–2 μm.

Author Contributions

J.L. designed the experiments and performed data analysis. S.L., Y.P. and K.L. carried out the experiments. Y.K. worked on XRD analysis of the materials. J.K. and B.M. worked on HRTEM observation. J.L. and P.J. co-wrote the paper.