22nd International Symposium on Plasma Chemistry July 5-10, 2015; Antwerp, Belgium Synthesis of carbon nanowalls by plasma-enhanced chemical vapor deposition and their rapid intercalation behaviour as lithium ion capacitor anode material A.D.C. Permana, A. Kameyama, M. Suzuki and S. Mori Department of Chemical Engineering, Tokyo Institute of Technology, Tokyo, Japan Abstract: The author reported the deposition of carbon nanowalls (CNWs) by plasmaenhanced CVD in CO/H 2 microwave gas discharge system without any catalyst. The electrochemical properties and morphology are analyzed. Deposited CNWs sample perform better electrochemical performance at high current density than graphitic material sample. The discharge capacity was measured 80.27, 64.31, 45.47, and 32.36 mAh/g at 6, 10, 15, and 20 C-rate respectively. This electrochemical performance stimulates the usage of CNWs as Li-ion capacitor (LIC) material for fast-charging device. Keywords: microwave plasma CVD, CNWs, LIC 1. Introduction Development of the capacitor technology has reached a certain point to improve the energy density which is the main drawback compared to Li-ion batteries (LIB) technology. The hybrid system of supercapacitor and LIB, or so-called Li-ion capacitor (LIC), is expected to fill the gap between those two earlier mentioned devices in a Ragone plot. In the development of LIC technology, it employs graphite for anode material and activated carbon as for cathode. Graphite was selected as an anode material of LIB because it has more negative potential than when intercalated by Li-ion and Li 4 Ti 5 O 12 environmentally benign. However, the SEI formation prevents cathode to fully discharged resulting irreversible capacity loss. To solve this problem, anode then predoped by Li-ion to reduce the capacity loss. Decreasing particle size into nano-scale may establish the transport kinetics between Li-ion and electron and enhance the electrode-electrolyte interphase area which also improves electrochemical properties. But even so, some drawbacks such as low electrode integrity and volumetric energy hold the system to achieve the highest performance. In the recent years, many groups have developed some approaches to use unordinary material for the electrode. The purpose of course is to improve the performance of the LIC, particularly by means of the energy density to be more like LIB [1-5]. Carbon nanowalls (CNWs) is well known as 2dimensional network of stacked grapheme layer on a substrate with several nanometers of thickness. Their unique properties, i.e. large surface area, chemical stability, mechanical strength, and high conductivity [6], draw many attentions for researches which are now developed for applications of field emission electron [7], sensor [8], fuel cell [9], capacitor [10], and LIB [11]. Through many studies, CNWs can be fabricated by various methods such as microwave plasma [12], radio frequency (RF) plasma [13], hot filament chemical vapor deposition (CVD) [9], sputtering [14], and so on. Most of P-II-5-16 them, the gas plasma used is CH 4 and H 2 . Among those methods, CVD assisted by microwave plasma is found very attractive because the operating temperature can be lowered and the possibility of no-catalyst process is very high [15]. In our group, CNWs growth by microwave plasma CVD without any catalyst and substrate pre-treatment has been developed by using CO as carbon source and H 2 gas plasma [16]. This study describes first use of CNWs as anode material for LIC application. 2. Experimental CNWs were prepared by a microwave plasma CVD system utilizing CO/H 2 gas plasma discharge similar with our previous studies [17]. Fig. 1. Experimental apparatus for microwave plasma CVD. Commercial LIC-grade Cu foil with 1 cm2 area is placed inside of a 15 mm inner diameter quartz discharge tube without any catalyst or pre-treatment flowed by CO and H 2 gas plasma connected by a modified ASTeX DPA25 plasma applicator. The operating condition of CNWs deposition process were as follows: total gas flow rate, 50 sccm: CO flow rate, 46 sccm; H 2 flow rate, 4 1 sccm; total pressure, 250 Pa; microwave plasma discharge power, 80 W; deposition time, 7 min. Electrochemical properties of all the samples were measured by using a Swagelok type two-electrode test cell system. Sample was placed at the bottom as the anode followed by monolayer polypropylene separator of Celgard 2400, and 16 mm φ Li foil purchased from Honjo Metal Co. Ltd. as the cathode. Electrolyte used in this study is 1M LiPF 6 in ethylene carbonate/dimethyl carbonate (EC/DMC, 1:1 by volume) purchased from Ube Industries, Ltd. VersaSTAT3 potentiostat/galvanostat electrochemical system was used to observe cyclic voltammetry (CV) and constant-current constant-voltage (CCCV) charge-discharge. The morphology of deposited CNWs film was characterized using scanning electron microscope (SEM, Hitachi S-4500) and transmission electron microscope (TEM, JEOL JEM-2010F). 3. Results and Discussion Deposited CNW on Cu foil was produced by microwave plasma system written above at deposition time 7 min is compared to graphitic carbon material (labelled as CNW and C). CCCV performs the charging of Li ion into CNW sample at 37.2 mAh/g (0.1 C-rate) then having discharge curves as the responds at 2.23, 3.72, 5.58, and 7.44 A/g (correspond to 6, 10, 15, and 20 C-rate) in the potential range of 0.1-2 V vs. Li+/Li as shown in Fig. 2a. The comparison CNW sample to C sample measured was shown in Fig. 2b. It can be deducted that C sample has better performance at low C-rate as 92.81 mAh/g at 0.1C than CNW as 85.10 mAh/g. When it comes to high Crate, however, the discharging performance of C sample decreases as the C-rate increases to 6 C (44.25 mAh/g) and 20 C (15.95 mAh/g). On the other side, CNW sample can maintain their performance up to 80.27 and 32.36 mAh/g as it was measured at 6 C and 20 C respectively. The effect of surface area increase by means of CNWs shape can enhance the electrochemical capacitance [10, 18]. This CNWs sample could be suitable material for fast charge-discharge device because of this superior high Crate behaviour. In Fig. 3a and 3b, the SEM and TEM images of CNW layer by deposition time of 7min after charge-discharge process was presented. The height of the deposited wall measured is about ~ 17 μm and the thickness is about ~ 18 nm. As it can be seen from the images, the wall shapes are maintained even after many times of charge-discharge cycling process which can be compared to our previous result [17]. Fig. 2. (a) Discharge profile of CNW sample at various C-rate, and (b) Discharge capacity of all samples at various C-rate. Fig. 3. (a) SEM and (b) TEM images of CNW sample after n cycle. 2 P-II-5-16 4. Conclusion CNWs deposited by microwave plasma CVD were successfully measured their electrochemical performance for capacitor application, in this study, LIC. Deposited CNWs suggested to be very good materials for rapidcharging device referring to its discharge capacity at high C-rate (20 C) by 32.36 mAh/g when compared to graphitic material sample of 2.12 mAh/g. 5. References [1] S. R. Sivakkumar, J. Y. Nerkar, and A. G. Pandolfo, Electrochimica Acta, 55, 3330 (2010) [2] J. H. Lee, W. H. Shin, M.-H. Ryou, J. K. Jin, J. Kim, and J. W. Choi, ChemSusChem, 5, 2328 (2012) [3] S.O. Kim, H. S. Kim, and J. K. 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