A new method of growing graphene on Cu by hydrogen etching

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A new method of growing graphene on Cu by hydrogen etching Linjie zhan version 6, 2015.05.12--2015.05.24 CVD graphene Hydrogen etching Anisotropic Copper-catalyzed Highly anisotropic hydrogen etching method for chemical vapor deposited (CVD) graphene catalyzed by the copper substrate. By exposing CVD graphene on copper foil to hydrogen flow around 800, the initially continuous graphene can be etched to have many hexagonal openings. Graphene, a two-dimensional, honeycomb arrangement of carbon atoms,has drawn significant attention with its interesting physical properties. In terms of the preparation of graphene, chemical vapor deposition (CVD) has raised its popularity as a scalable and cost-effective approach for graphene synthesis.

In this work, we have studied anisotropic hydrogen etching of chemical vapor deposited graphene as the reverse reaction of graphene growth. We observed that continuous graphene could be etched into hexagonal openings by exposing CVD graphene on copper foil to hydrogen flow at high temperatures. The etching is found to be temperature-dependent, and 800 offers the most efficient and anisotropic etching. Of the angles of graphene edges after etching at 800, 80% are 120. Moreover, we observed that copper played an important role in catalyzing the etching reaction, as no etching was observed for graphene transferred to Si/SiO 2 substrate under similar conditions. This highly anisotropic hydrogen etching technology may work as a simple and convenient way to determine graphene grain size and crystal orientation and may enable the etching of graphene into nanoribbons with smooth and ordered zigzag edges without compromising the quality of graphene. Our work started with the preparation of CVD graphene. After the synthesis of CVD graphene, anisotropic etching of graphene was done in the same CVD chamber at 800 with the flow of hydrogen. As illustrated in Figure 1, the etching reaction is the reverse reaction of graphene growth, as hydrogen can react with carbon in graphene and produce methane. We observed that almost every etched hexagon had a particle in the center, as

shown in the left SEM image in Figure 1 (a). The particles are believed to come from the quartz tube used in the CVD chamber, and the etching reaction is initiated by breaking the carbon-carbon bond of graphene in locations they were deposited. Energy-dispersive X-ray spectroscopy has been performed to test the composition of the particles. Strong silicon and oxygen peaks from the spectrum taken on one of the particles indicate that the particles are silicon dioxide. Figure 1. (a) SEM image of graphene after etching on copper foil (b) transferred onto a Si/SiO 2 substrate. After small openings were etched on graphene, the copper substrate underneath would serve as a catalyst for hydrogen to react with carbon in graphene and, hence, accelerate the etching reaction of graphene. Interestingly, the catalytic etching reaction is highly anisotropic in our experimental conditions. As shown in the SEM image in Figure 1(b) taken

of the graphene transferred to a Si/SiO 2 substrate, the openings in graphene after etching turn out to be very regular hexagonal shaped, and edges with 120 angles can be found in many etched corners. While we report hydrogen etching of graphene on a copper substrate in this paper, a similar reaction may occur for graphene on other substrates such as nickel. Even though the SiO 2 nanoparticles in our current work are randomly located, controlled positioning of SiO 2 nanoparticles can be achieved by combining patterning and deposition of SiO 2 particles. For instance, by using assembled nanospheres as a shadow mask for SiO 2 deposition, one should achieve SiO 2 particle deposition at desired locations. Alternatively, our observed hydrogen etching of graphene may also work after initiating openings in graphene via patterning and oxygen plasma etching. We have conducted micro-raman microscopy on both as-grown CVD graphene and graphene after the etching reaction. As-grown graphene was transferred onto a 300 nm Si/SiO 2 substrate using the reported transfer technique. As shown in the SEM image after transfer in Figure 2(a), the graphene is continuous, clean, and uniform over a large area. Raman spectra were collected over the entire substrate to determine the number of layers, as well as the quality of graphene.

Figure 2. CVD graphene before and after etching. (a) As-grown CVD graphene transferred onto Si/SiO 2 and a representative Raman spectrum as an inset; (b) graphene etched by H 2 at 800 and transferred onto Si/SiO 2. Raman spectra (inset) show the intact graphene (pointed by red arrow) and etched region (pointed by blue arrow). The inset of Figure 2(a) shows a typical Raman spectrum of the astransferred graphene. The absence of a D peak indicates that the graphene after transfer maintains high quality. Figure 2(b) shows the SEM image of graphene etched at 800 after transfer. Raman spectra were taken from the remaining graphene and one of the etched hexagons, respectively. The red curve in the inset of Figure 2(b) represents the Raman spectrum of the remaining graphene (pointed by the red arrow), which does not show the presence of a D peak, indicating the remaining graphene after etching has few defects. The blue curve represents the Raman spectrum inside the etched hexagons (pointed by the blue arrow), which almost does not show any G

and 2D band intensity, indicating the removal of graphene by anisotropic etching of hydrogen. Temperature always plays a significant role in chemical reactions. For a better understanding of the etching process, we studied the influence of temperature in the catalytically etching reaction. Four different temperatures were investigated in our experiment. The SLG samples used in the etching experiments were prepared in the same round of growth reaction, ensuring the uniformity and consistency of the starting SLG in each etching reaction. Figure 3. SEM images at different magnifications of graphene etched at different temperatures and transferred onto a Si/SiO 2 substrate: (a and b) 700 ; (c and d) 800. After etching at 700 for 30 min, the etching was observed to be mild and is probably along the grain boundaries of graphene, therefore leading to graphene islands, shown in Figure 3(a) and b using different magnifications.

Only a small amount of etched hexagons is observed inside the graphene islands after etching at 700 for 30 min. When 800 was used for etching, a larger area of graphene was etched away, and the etched patterns were mostly hexagonal, as seen in Figure 3(c) and (d). We could also observe that the edges of etched graphene were mostly 120 in Figure 3(d). While we report hydrogen etching of graphene on a copper substrate in this paper, a similar reaction may occur for graphene on other substrates such as nickel. Even though the SiO2 nanoparticles in our current work are randomly located, controlled positioning of SiO2 nanoparticles can be achieved by combining patterning and deposition of SiO2 particles. For instance, by using assembled nanospheres as a shadow mask for SiO2 deposition, one should achieve SiO2 particle deposition at desired locations. The red curve in the inset of Figure 2 represents the Raman spectrum of the remaining graphene (pointed by the red arrow), which does not show the presence of a D peak, indicating the remaining graphene after etching has few defects.

Alternatively, our observed hydrogen etching of graphene may also work after initiating openings in graphene via patterning and oxygen plasma etching. Methods Graphene growth was done using copper foil (99.8%, Alpha Aesar) as a substrate. Copper foil was loaded into a 2 in. fused quartz tube and heated to 1000 with the flow of 7 sccm H 2 at 40 mtorr. The Cu foil was then annealed at 1000 for 20 min. Seven sccm CH4 and 30 sccm H 2 were introduced to the CVD system at 500 mtorr for 30 min for graphene growth. The temperature was decreased to 600 without changing flow rates and pressure. CH 4 was then turned off at 600, and the system was cooled to room temperature with the flow of 30 sccm H 2 at 500 mtorr. Anisotropic etching of graphene by hydrogen was done in the same CVD chamber as graphene growth, with the flow of 30 sccm H 2 at 500 mtorr, and the etching was carried out for 30 min at 800. Conclusion After small openings were etched on graphene, the copper substrate underneath would serve as a catalyst for hydrogen to react with carbon in graphene and, hence, accelerate the etching reaction of graphene.

Interestingly, the catalytic etching reaction is highly anisotropic in our experimental conditions. As shown in the SEM image in Figure 1 taken of the graphene transferred to a Si/SiO2 substrate, the openings in graphene after etching turn out to be very regular hexagonal shaped, and edges with 120 angles can be found in many etched corners. We also studied the orientation of the etching by measuring the angles of graphene edges after etching. As shown in Figure 2, 80% of the measured angles were 120, indicating that the etching is along the specific crystal orientation of graphene. Temperature always plays a significant role in chemical reactions. For a better understanding of the etching process, we studied the influence of temperature in the catalytically etching reaction. Four different temperatures were investigated in our experiment. Acknowledgements

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