July 14, 2024

Flex Tech

Innovation in Every Curve

Deformable micro-supercapacitor fabricated via laser ablation patterning of Graphene/liquid metal

Fabrication process for deformable micro-supercapacitors

Figure 1a shows an illustration of integrated soft electronic system, comprising deformable MSC array and wearable electronic device. Deformable MSC array is prepared as follows. First, EGaIn was coated onto the SEBS substrate using a brush (Fig. 1b). Despite the high surface tension of EGaIn, a uniform EGaIn film was obtained after brushing. The resulting EGaIn film exhibits excellent electrical properties, which is effectively used as a current collector (Supplementary Fig. 1). Then, graphene was selectively deposited onto desired regions of EGaIn film by screen-printing of graphene paste with a pre-designed stencil (Supplementary Fig. 2), resulting in graphene/EGaIn bi-layer (Fig. 1b). Next, a laser is irradiated along the pre-designed path to fabricate the pattern. When the laser is irradiated, graphene/EGaIn and EGaIn along the path of the laser are ablated, resulting in interdigitated graphene/EGaIn pattern and EGaIn circuit, respectively. On the other hand, the laser does not affect the SEBS substrate because it barely absorbs the laser wavelength (355 nm) (Fig. 1c); thus the deformable characteristics of SEBS substrate is maintained. Then, poly(vinylidene fluoride-co-hexafluoropropylene) based ion gel was coated onto the interdigitated electrode region to complete MSCs. The field-emission scanning electron microscopy (FE-SEM) images of the laser ablated graphene/EGaIn and EGaIn are shown in Fig. 1d, e, respectively. An LED was connected to the MSC circuit (Fig. 1f). In addtition, various deformable patterns on graphene/EGaIn and EGaIn were easily fabricated on the SEBS, e.g., the institute logo (Fig. 1g) which accommodates easily a large mechanical deformation (Fig. 1h).

Fig. 1: Fabrication process for deformable micro-supercapacitors.
figure 1

a Illustration of an integrated system comprising soft-electronics and deformable energy storage component. b The fabrication process of EGaIn-based MSC. c UV-vis spectra of SEBS, EGaIn, and graphene. FE-SEM images of laser ablated d Graphene/EGaIn and e EGaIn (Scale bar = 200 µm). Photographs of f institute logos, g deformed logos, and h an LED connected to the MSC circuit (Scale bar = 1 cm).

Optimization of laser ablation conditions

Even though SEBS barely absorbs the laser wavelength (355 nm), the heat generated during the laser ablation of graphene and EGaIn could potentially affect the SEBS. In addition, an intense laser could potentially cause damage to the SEBS. Consequently, we optimized the laser ablation process to ensure the complete ablation of both graphene and EGaIn without any damage on the SEBS. Figure 2a illustrates pulse energy (E) change with pulse duration (τ). Here, we fixed the peak power (Ppeak) and laser frequency at 3.9 W and 100 kHz, respectively, while τ was adjusted from 8500 ns to 4000 ns. Because EPpeak · τ38,39, E decreases with reducing τ at fixed Ppeak. Figure 2b shows the state of the sample after laser ablation at different τ and the number (N) of the laser scan. The corresponding optical microscopy (OM) images are shown in Supplementary Fig. 3. Despite a very low laser absorption of the SEBS, a long pulse duration (τ = 8500 ns) caused severe damages (burned and even cut) on the SEBS (Supplementary Fig. 4). Regardless of N, the gap size after laser ablation decreases with decreasing τ. When τ is shorter than 7000 ns with a single scan, only graphene undergoes ablation, but EGaIn does not remove. On the other hand, at N = 2 and 3, a complete EGaIn ablation was achieved even at τ = 5500 ns. We conclude that two scans of a laser with τ of 5500 ns is the optimal condition, where there is no damage on the SEBS and the narrowest gap size ( ~ 90 µm) is achieved. This value is much smaller than that ( ~ 1000 µm) reported in the literature on printed EGaIn-based MSCs35,40.

Fig. 2: Laser ablation optimization.
figure 2

a Pulse energy dependence on the pulse duration. b Sample state after laser ablation as functions of pulse duration and the number of the lase scan (red region: damaged SEBS, green region: the entire ablation of both graphene and EGaIn without any damage on SEBS, and gray region: only graphene ablation but not EGaIn).

Mechanical stability of EGaIn/Graphene electrode

Figure 3a shows photographs of graphene/EGaIn electrode during a single stretching and releasing at two different strains (20 and 50%) without and with the ion gel. In the absence of the ion gel, several large cracks were generated in the graphene layer during stretching regardless the strain, causing the graphene layer to clump and lose its original shape during the releasing process. Furthermore, the cracked graphene even peeled off from the EGaIn layer at 50% strain. This is attributed to a large difference in the tensile modulus between the brittle graphene layer and the EGaIn layer. On the other hand, in the presence of the ion gel, small cracks occurred uniformly in the graphene layer during stretching regardless strain. Nevertheless, the graphene layer was almost restored to its original shape except the trace of the cracks. This is attributed to the partial infiltration of the soft ion gel into the graphene layer (Fig. 3b), providing reliable adhesion to the EGaIn layer. Furthermore, there was no peeling off of the graphene layer even after 1000 cycles of repeated 20% stretching, indicating that the ion gel maintained a stable mechanical interface with the EGaIn layer (Fig. 3c). However, when stretching increases to 50%, a cracking occurred in the ion gel layer (Supplementary Fig. 5), causing the graphene layer to lose its original shape and eventually delaminate even after 100 cycles. Therefore, we conclude that a stable charge transport between graphene and EGaIn can be maintained up to 20% stretching.

Fig. 3: Mechanical stability against stretching and releasing of graphene/EGaIn electrode.
figure 3

a Photographs of graphene/EGaIn electrode during a single stretching and releasing at two different strains (20% (left) and 50% (right)) without and with the ion gel (Scale bar = 1 cm). b Schematic of the roles of the ion gel during mechanical stretching. c Photographs of graphene/EGaIn electrode during repeated stretching and releasing at two different strains (Scale bar = 1 cm) (20% (left) and 50% (right)).

Tailoring gap size of MSCs

Because the rate performance and areal capacitance of the MSCs strongly depend on the gap size between neighboring interdigitated electrodes, we prepared three gap sizes (100, 180, and 500 µm) by adjusting a laser ablation path. Figure 4a shows the photograph of the fabricated MSCs with different gap sizes. Hereafter, the samples were denoted based on the gap size. For example, 500-MSC corresponds to MSC with a gap size of 500 µm. Electrochemical impedance spectroscopy (EIS) was performed at a frequency ranging from 100 kHz to 10 mHz. According to the Nyquist plots shown in Fig. 4b, as the gap size decreases, the slope in the low-frequency region increases, which means better ion diffusion kinetics within the electrode materials. The diffusion coefficient (D) of lithium ion calculated from the Warburg region (inset of Fig. 4b) for 100, 180, and 500-MSC is 2.02 × 10−4, 6.21 × 10−5, and 3.05 × 10−5 cm2 s−1, respectively. We also investigated the dependence of phase angle on the frequency of all MSCs (Fig. 4c). The relaxation time constant (τ0) of MSCs, which is the minimum time required to completely discharge all the stored energy with an efficiency of over 50%, is calculated as the inverse of the characteristic frequency (f0) (that is, the frequency at a phase angle of 45°). The value of τ0 for 500, 180, and 100-MSC are 6.3, 4.0, and 2.0 ms, respectively, suggesting faster ion kinetic with decreasing gap size.

Fig. 4: Energy storage performance of MSCs.
figure 4

a Photographs and OM images of three MSCs with different gap sizes (Scale bar = 5 mm). b Nyquist plots of MSCs. (inset: Z’ as a function of ω−1/2 plot in low frequency range). c Bode angle plots of MSCs. d CV curves of MSCs at 50 mV s−1. e GCD curves of MSCs at 2 µA cm−2. f Areal capacitances in the current density range from 2 to 30 µA cm−2. g CV curves of MSCs based on different graphene layers. h Nyquist plots of MSCs. i Areal capacitance vs current density of MSCs based on different graphene layers.

To investigate the electrochemical behavior of the MSCs, we measured the cyclic voltammogram (CV) curves at 50 mV s−1 (Fig. 4d). The CV curves of all MSCs exhibit a quasi-rectangular shape, indicating electric double layer (EDL) behavior arising from adsorption/desorption of ions into graphene layers40. The curves widened as the gap size decreased, suggesting that MSCs with smaller gap sizes can store more charges. This is simply because the loading amount of graphene per unit area increases with decreasing gap size. This behavior is also confirmed in galvanostatic charging/discharging (GCD) profiles (Fig. 4e). As the gap size decreased, the charging/discharging duration of the GCD profiles increased without distorting the symmetrical shape. Based on the GCD curves at various current densities (Supplementary Fig. 6), the areal capacitance at a current density of 2 µA cm−2 of 100-MSC was 328 µF cm−2, which is higher than those of 180-MSC (160.8 µF cm−2) and 500-MSC (78.24 µF cm−2). Moreover, 100-MSC maintained 77% areal capacitance even at a 15-fold higher current density (30 µA cm−2), showing a superior rate capability compared to 180 and 500-MSCs, which retained only 37.6 and 29.9%, respectively (Fig. 4f).

Tailoring electrode thickness of MSCs

To further enhance the areal capacitance of 100-MSC, we controlled the graphene mass loading by multiple coating graphene paste (Supplementary Fig. 7). The MSCs were denoted on the basis of the number of the graphene layer (n). For example, 3L-100-MSC is composed of a 3-layer graphene film with a gap size of the interdigitated pattern having 100 µm. As n increased, the current increased at a given scan rate (50 mV s−1), while the CV curves are slightly distorted (Fig. 4g). This is since the horizontal graphene sheet alignment results in low out-of-plane electrical conductivity and the resistance on the graphene film increases with increasing film thickness41. This is also supported by Nyquist plots in Fig. 4h. The semicircle in the high-frequency region was enlarged with increasing n, which is attributed to higher charge transfer resistance. Based on the measured GCD profiles at various current densities (Supplementary Fig. 8), the areal capacitance was extracted (Fig. 4i). The 3L-100-MSC exhibited the areal capacitance of 1336 at 2 µA cm−2 and 705 µF cm−2 at 30 µA cm−2. Also, the value at all current densities are higher than others (2L-100-MSC and 1L-100-MSC). But, the rate capability (52.7%) of 3L-100-MSC is lower than others (69.1% of 2L-100 MSC and 77.0% of 1L-100-MSC). This is because, with increasing electrode thickness of MSCs, a large amount of charge could be stored in the device, but the inefficient electron transport through the entire electrodes makes the rate performance poor. Nonetheless, owing to the narrow gap size of the 3L-100-MSC, a better rate performance could be achieved compared to MSCs with one layer but a large gap (1L-500-MSC (29.9%) and 1L-180-MSC (37.6%)). Also, a long cycle life for practical application was achieved (Supplementary Fig. 9). A decrease of only 9.5% of the first run was recorded after 10,000 cycles.

MSCs operation under mechanical deformations

The major requirement for a deformable energy storage device is to maintain the energy storage performance under various mechanical deformations. In this study, folding and stretching are selected for 3L-100-MSC for the deformability test (Fig. 5a). Figure 5b shows the CV curves under folding and 20% stretch. The CV curves under both cases remain almost the same, indicating the stable electrochemical behavior under mechanical deformation. Moreover, the GCD curves measured under mechanical deformations showed almost the same as that without deformation (Fig. 5c). Figure 5d compares the areal capacitance as a function of the current density under different deformation states, demonstrating that excellent performance stability (95 and 91% under folding and stretching, respectively). To operate deformable electronics reliably, energy storage components should maintain the energy storage performance not only in the deformed state but also after recovery state. We performed the cycle test with repetitive deformations (Fig. 5e). Regardless of the deformation type, we observed ~90% capacitance retention after 1000 cycles, indicating that interdigitated graphene/EGaIn electrode on the SEBS sufficiently accommodated repetitive mechanical deformation and recovery. During repeated stretching and releasing at 20% strain, the small cracks and clumped region occurred at both the ion gel and the graphene layer. These structural deformations probably reduce the electrochemical properties (Supplementary Fig. 10). Thus, we believe that the cycle stability of MSCs can be further improved by employing the mechanically durable ion gel.

Fig. 5: The energy storage performance under various mechanical deformations.
figure 5

a Photographs of MSC under various mechanical deformations. b CV curves and c GCD profiles under different mechanical deformations. d Areal capacitance. e Capacitance retention with repetitive mechanical deformations.

MSC array integration with electronics

To demonstrate MSC as a power source for a soft electronic system, we integrated the MSC array with LEDs (Fig. 6a). To meet the LED’s operating voltage requirement and stable operation, we designed an MSC array consisting of 3 series and 3 parallel connections. To this end, we coated EGaIn on a large-area SEBS substrate and partially loaded graphene on coated EGaIn through screen printing. Next, nine interdigitated electrodes and the EGaIn circuits connecting them were prepared using laser ablation. Finally, MSC array was completed by coating ion gel on the interdigitated electrode area. The area of fabricated MSC array was 35 cm2 (7 cm × 5 cm). The MSC array exhibited a wide CV curve and a 3-fold increase in operating voltage compared to a single arrayed MSC (Fig. 6b). Moreover, the shape of CV curve does not show any distortion, indicating stable electrochemical behavior. Figure 6c shows the GCD profiles of single MSC and MSC array. MSC array showed a 3-fold increase in charging/discharging duration and operating voltage, implying increased output energy and power (Fig. 6c). These results indicate that laser ablation enables a facile fabrication of MSC array in a large area (Supplementary Fig. 11). In addition, the high conductivity of the EGaIn current collector was achieved even though it was fabricated by brushing method to cover a large device area. Finally, when two LEDs were connected to the MSC array through the EGaIn circuit, they stably operated under various mechanical deformations, including stretching, twisting, folding, and wrinkling (Fig. 6d). Furthermore, even with just two MSCs connected in series, various electronics could be operated (Supplementary Fig. 12).

Fig. 6: Fabrication of MSC array and miniaturization of MSC.
figure 6

a Photograph of nine MSC units connected in three parallel and three series. b CV curves and c GCD profiles of single MSC and multiple MSC array. d Photographs of the MSC array integrated with two LEDs circuit under various mechanical deformations (Scale bar = 5 cm). e Photographs of the downsized MSC units (Scale bar = 0.5 cm). f CV curves at 50 mV/s and g GCD profiles at 2 µA/cm2 of the downsized MSCs. h Photograph of three serially connected MSC units of a downsized area (0.5 cm2) integrated with LED circuit under bending (Scale bar = 2 cm).

Miniaturization of MSCs

Utilizing the high-resolution patterning capability of laser ablation, we successfully downsized the MSCs. While maintaining a gap size, we fabricated smaller MSCs with total sizes of 0.5 cm2 and 0.25 cm2 (Fig. 6e). As the gap size remained constant, the amount of loaded graphene on per unit area is identical. Consequently, all samples exhibited nearly identical electrochemical behaviors (similar CV curves) (Fig. 6f). Moreover, almost identical charging/discharging durations were observed regardless of MSC size (Fig. 6g), indicating the reliable energy storage performance of downsized MSCs. Lastly, we demonstrated the operation of an LED by using three serially connected MSC units of a downsized area (0.5 cm2) under bending (Fig. 6h).

In summary, we fabricated deformable MSCs by using laser ablation technique. To optimize the energy storage performance, we tailored the gap size of the interdigital electrodes and the mass loading of graphene. The fabricated MSC exhibited a high areal capacitance (1336 µF cm−2) with reliable rate performance. Remarkably, the MSC retained the energy storage performance under various mechanical deformations due to the intrinsic liquid state of EGaIn current collector and the highly flexibility of SEBS substrate. To demonstrate the feasibility of MSCs as a deformable power source, we fabricated a soft electronic system comprising serial and parallel connected MSC array and LEDs. The obtained soft electronic system stably operated under various mechanical deformations (e.g., folding, stretching, wrinkling, and twisting). To increase further the stretching of MSCs, a highly mechanical durable ion gel such as polystyrene-b-poly(methylmethacrylate)-b-polystyrene copolymer is desirable. As the laser ablation technology can easily be utilized to pattern various electrode materials including carbon materials, metal oxides, and Mxene, this could be applied for highly deformable and high-performance energy storage systems.

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