Patterned Si thin film electrodes for enhancing structural stability
© Cho et al; licensee Springer. 2012
Received: 27 September 2011
Accepted: 5 January 2012
Published: 5 January 2012
A patterned film (electrode) with lozenge-shaped Si tiles could be successfully fabricated by masking with an expanded metal foil during film deposition. Its electrochemical properties and structural stability during the charge-discharge process were examined and compared with those of a continuous (conventional) film electrode. The patterned electrode exhibited a remarkably improved cycleability (75% capacity retention after 120 cycles) and an enhanced structural stability compared to the continuous electrode. The good electrochemical performance of the patterned electrode was attributed to the space between Si tiles that acted as a buffer against the volume change of the Si electrode.
Keywordspatterned electrode silicon film stress anode
The secondary Li-ion batteries with a high energy density have gained attention from wide-range applications of power source for the portable electronics, electric vehicle, and electric storage reservoir. In order to increase the energy density in the limited battery volume, the volume of the cathodic electrode having Li sources should be increased, whereas that of the anodic electrode has to be decreased, that is, anode materials with high theoretical capacity are needed to store the large amount of Li ions.
For the anodic materials, some of the candidates are Si, Sn, Al, Ge, and compounds including these elements [1, 2]. Si has a much higher specific energy (4,200 mAh/g for Li4.4Si) than commercial graphite (372 mAh/g for LiC6). However, there is a severe practical problem in the application of Si electrodes, i.e., when Si is used as an anode material for Li-ion batteries, a large volume expansion/shrinkage occurs during the charge-discharge (lithiation-delithiation) process. The volume change of Si (310%) causes surface cracking and pulverization of the Si film and leads to a rapid capacity fade during initial cycles. The poor electrochemical performances are ultimately caused by repetitive mechanical stress accompanied by large volume changes . Until now, many attempts have been made to prolong the cycle life of Si film electrodes [4–9]. Most researches focused on enhancing the adhesion between the Si film and a current collector (substrate) because the amount of Li storage was limited and the generation of stress was restrained by the enhanced adhesion.
In this article, the electrochemical properties of the continuous and patterned Si film electrodes are examined, and the improved cycle performance of the patterned electrode is discussed by observing the surface morphologies after 10 cycles.
A patterned Si film was fabricated by using an expanded metal foil (stainless steel) with lozenge-patterned holes (THANKS-METAL, Japan) as a mask. A continuous (conventional) Si film electrode was also fabricated for comparison. The Si films were deposited on a Cu foil substrate using DC magnetron sputtering systems. Prior to the deposition, the Cu substrate was ultrasonically cleaned and annealed in vacuum-sealed ampules at 573 K for 30 min to remove the residual impurity gases at the surface. The films were grown in a vacuum chamber under a pressure of 5 × 10-3 Torr in argon atmosphere. A cross-sectional analysis was performed to measure thickness of the film with an alpha-step profiler. The thickness of the Si film fabricated in this study was 350 nm.
Crystallinity and surface morphology of the two Si films were investigated by means of transmission electron microscopy [TEM], X-ray diffraction [XRD], and field emission scanning electron microscopy. Although the stress generated during the electrochemical test was indirectly traced by analyzing the broadness of the substrate peaks, a clear distinction before and after the test was difficult.
Electrochemical measurements were preformed in CR2032 coin cells with the different Si film electrodes. A metal lithium foil was used as a counter electrode. Electrolyte was made from 1 M LiPF6 in a 1:1 (v/v) mixture of ethylene carbonate and dimethyl carbonate. The separator used was a porous polypropylene (Celgard 2400; Celgard, Charlotte, NC, USA). Galvanostatic charge-discharge half-cell tests were performed at a current density of 2,100 mA/g (0.5C-rate) at ambient temperature. The test was conducted between the initial OCV and 0.01 V versus Li/Li+, then between 0.01 and 1.2 V after the first cycle. Charge-discharge measurements were performed with a constant current. For the calculation of capacity, the mass of the Si electrode is derived from its density, 2.33 g/cm2, assuming the crystalline structure.
Results and discussion
However, weak peaks of CuO are observed in Figures 3a and 3b. The formation of CuO can be confirmed in the inset of Figure 3a where peaks corresponds to (111) and (200) planes of CuO (JCPDS 80-1719), respectively. The CuO layer seems to form on the surface of the Cu substrate during the annealing process. The intensity of CuO peaks decreases at the patterned Si film and almost disappears at the continuous Si film. This is acceptable because the Si-covered area for the continuous film is wider than that for the patterned film.
At the first cycle, 2,890 mAh/g of charge capacity and 2,200 mAh/g of discharge capacity were obtained from the continuous electrode (Figure 4a), and 3,620 mAh/g and 2,200 mAh/g capacities were obtained from the patterned electrode (Figure 4b). The relatively high charge capacity of the patterned electrode is mainly related to an electrochemical reaction between Li and Cu oxide layers partially exposed on the surface. It had been already reported that the reaction occurred at a voltage range of 1.7 V to 1.0 V and then formed LixCuO . In addition to this, another reason is the solid electrolyte interphase formation that is sensitive to the surface morphology of the electrode because the patterned electrode has a wider surface area than the continuous electrode . These reaction products lead to the capacity loss at the first cycle, and thus a low coulombic efficiency ((discharge capacity/charge capacity) × 100(%)) of 60% was obtained at the first cycle as shown in Figure 4b. However, the patterned electrode exhibits higher efficiencies than those of the continuous electrode which were obtained after the first cycle.
However, it can be found that the size of the Si tile was slightly increased after cycling (Figure 2b and 6b), and relatively small cracks were generated in the patterned electrode. Unfortunately, these results indicate that the volume change of Si was completely not reversible during the repeated cycling. Therefore, it is concluded that the space between tiles in the patterned Si electrode buffers the volume change of Si during the charge-discharge process and partially disperses the stress generated in the Si electrode. In the next work, it is expected that electrochemical properties of the patterned electrode fabricated on a substrate without an oxide layer will be highly improved because the adhesion between a film and a substrate will be enhanced by the surface treatment of the substrate. Because of this, the study on a surface-etched substrate is in progress.
A patterned Si film (electrode) with lozenge-shaped tiles could be successfully fabricated by masking with an expanded metal foil, and its electrochemical properties were compared with those of a continuous (conventional) film electrode. The patterned electrode exhibits a remarkably improved cycleability compared to the continuous electrode with 75% capacity retention after 120 cycles. After 10 cycles, the continuous Si film with severe cracks was partially detached from the substrate, whereas Si tiles in the patterned film still remained without severe damage. The good electrochemical performances of the patterned electrode were attributed to the space between Si tiles that acted as a buffer against the volume change of Si.
This research was supported by the Pioneer Research Center for Nano-morphic Biological Energy Conversion and Storage. This research was partially supported by the Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education, Science and Technology (2011-0024767).
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