High mass loading and fast charge transport are two crucial but often mutually exclusive characteristics of pseudocapacitors. On conventional carbon supports, high mass loadings inevitably lead to sluggish electron conduction and ion diffusion due to thick pseudocapacitive layers and clogged pores. Here we present a design principle of carbon supports, utilizing self-assembly and microphase-separation of block copolymers. We synthesize porous carbon fibers (PCFs) with uniform mesopores of 11.7 nm, which are partially filled with MnO2 of <2 nm in thickness. The uniform mesopores and ultrathin MnO2 enable fast electron/ion transport comparable to electrical-double-layer-capacitive carbons. At mass loadings approaching 7 mg cm−2, the gravimetric and areal capacitances of MnO2 (~50% of total mass) reach 1148 F g−1 and 3141 mF cm−2, respectively. Our MnO2-coated PCFs outperform other MnO2-based electrodes at similar loadings, highlighting the great promise of block copolymers for designing PCF supports for electrochemical applications.
High mass loading and fast charge transport are at the heart of electrochemical energy storage1,2,3. The former is crucial for high energy per device, and the latter for high power4. Low-cost, high-capacitance, and environment-benign pseudocapacitive MnO2 are loaded on electrically conductive supports and used as supercapacitor electrodes with a theoretical limit of 1367 F g−1 (based on a potential window of 0.8 V)5,6,7,8,9. Toward commercialization, the mass loading of the total active materials must be at least 5 mg cm−210. However, high mass loadings often lead to thick and dense layers of insulating MnO2 (10−5~10−6 S cm−1) on the supports11,12,13,14. Consequently, the internal resistance increases and the ion diffusion is perturbed, resulting in sluggish charge transport—both electron conduction and ion diffusion5,11,15. Here we innovate the design of porous carbon fiber (PCF) as a lightweight, flexible, binder-free, and conductive-additive-free support for MnO2. Using the disparate concept of block copolymer microphase-separation to generate uniform mesopores in PCFs, we have bridged the two mutually exclusive characteristics, i.e., high mass loadings and ultrafast electron/ion transport.
An ideal support for MnO2 and other transition metal oxides (RuO2, NiO, WO3, and Fe2O3, etc.) needs the characteristics of (1) lightweight, (2) large surface areas for high loadings, (3) high electron conductivity, and (4) low ion diffusion resistivity. However, there is not a single nanostructure that meets all these characteristics5,15. Carbon supports are inherently lightweight and electrically conductive. At high mass loadings of transition metal oxides, the electrical conductivity of electrodes decreases, but it can be restored by blending or wrapping with additional conjugated polymers16,17 or carbon additives16,18,19, as shown for excellent supports such as wearable textile structures16 and graphene16,20. The ion conduction, however, is drastically complicated21, and the efficient ion diffusion across the entire support, as well as the thick layer of MnO2, remains a significant challenge. To mitigate the ion diffusion resistivity, ultrathin layers of MnO2 have been deposited on model supports, e.g., nanoporous Au22,23, Pt foil9, Ni foil24, Si wafer25, dendritic Ni26 and macroporous Ni film27. With a thickness of <10 nm22 or at a mass loading of <0.35 mg cm−2 on the model supports23,26, MnO2 exhibits fast electron/ion transport and the gravimetric capacitances approach the theoretical limit. Nevertheless, when the conventional lightweight carbon supports are loaded with MnO2, they either suffer from a limited surface area for depositing a large amount of MnO2 thin layers (e.g., carbon cloth11,12, carbon fibers16,28,29,30 and other macroporous carbons13,14), or they lack desirable porous structures that facilitate rapid ion diffusion across long distances to maintain high rate capability (e.g., microporous carbons5,15,31).
Ultimately the key to high mass loading and fast electron/ion transport lies at the design of porous carbon architectures32,33. We hypothesize that mesoporous carbon fibers with a narrow pore size distribution are the most preferable for addressing the challenges of high mass loading and fast electron/ion transport. Conversely, micropores are susceptible to clogging after loading with MnO2 and thus provide sluggish ion transport, while macropores offer limited surface areas for high mass loadings of transition metal oxides. In addition, non-uniform mesopores lead to inefficient use of the surface area for depositing MnO2 and potential clogging of the small pores.
To test our hypothesis, herein we demonstrate block copolymer-derived PCFs as lightweight and high mass-loading supports for MnO2 (Fig. 1). Because block copolymers self-assemble and microphase separate into uniform and continuous nanoscale domains34,35,36,37,38,39,40,41, after pyrolysis they generate interconnected mesoporous carbons with large surface areas for depositing MnO2. Disparate from all other carbon supports, the mesopores are designed from the macromolecular level and offer a high degree of uniformity. Importantly, our judiciously designed mesopores have an average diameter of 11.7 nm and are partially filled with a <2-nm-thick layer of MnO2 (Fig. 1c). On the one hand, the remaining mesopores provide continuous channels for efficient ion transport across the entire electrode, significantly reducing the ion diffusion resistance. On the other hand, the fibrous carbon network provides expressways for efficient electron transport without the need for any conductive additives. This contrasts with hard-templated mesoporous carbon particulates (e.g., CMK-331), which demand polymer binders to hold the discrete carbon particulates together. At high mass loadings approaching 7 mg cm−2, the PCF-supported MnO2 electrodes (PCF@MnO2) show superior electron/ion transport and outstanding charge-storage performances.
To illustrate the crucial importance of uniform mesopores for high mass loading of MnO2, we have synthesized two types of carbon fibers, i.e., PCFs with uniform mesopores derived from poly(acrylonitrile-block-methyl methacrylate) (PAN-b-PMMA) and conventional carbon fibers (CFs) with limited mesopores from pure polyacrylonitrile (PAN). Scanning electron microscopy (SEM) shows the contrasting morphologies of PCFs and CFs (Fig. 2a, d and Supplementary Fig. 1). Owing to the microphase separation of PAN-b-PMMA and the subsequent degradation of poly(methyl methacrylate) (PMMA), the PCFs were perforated with a large number of uniformly distributed, randomly oriented, and interconnected mesopores of ~11.7 nm (Figs. 2a, 3a, and Supplementary Fig. 1a)42. In contrast, the CFs derived from PAN exhibited relatively smooth surfaces and no observable mesopores under SEM (Fig. 2d and Supplementary Fig. 1b). Small angle X-ray scattering (SAXS) spectroscopy confirmed the microphase separation of PAN-b-PMMA and revealed that the average center-to-center pore-spacing in PCFs was 25.7 nm (Supplementary Fig. 2). The volume fraction of PAN in PAN-b-PMMA was ~65%, and supposedly the block copolymer should self-assemble into either cylindrical or gyroidal structures, depending on the incompatibility of the two blocks. After pyrolysis, however, the porous carbon fibers showed no well-defined cylindrical or gyroidal structures but interconnected mesopores that were irregularly shaped and uniformly distributed, as shown in the cross-sectional SEM image (Supplementary Fig. 1a). This morphology is attributed to the crosslinking of PAN at elevated temperatures, which hindered the microphase separation of PAN-b-PMMA into well-defined cylindrical or gyroidal structures, similar to the crosslinking-induced hindering effect in previous reports43,44.
The two types of carbon fibers were immersed in aqueous solutions of potassium permanganate (KMnO4, 10 mM) at 80 °C to deposit MnO2 on their surfaces. We chose the solution-based redox deposition because it creates a conformal and homogenous layer of MnO2 inside the pores via a self-limiting redox reaction between KMnO4 and carbon32,45,46. Compared with electrochemical deposition (Supplementary Fig. 3), the redox reaction deposition is advantageous because it yields uniform and homogeneous layers of MnO2 on PCFs that ensure a low ion diffusion resistance and thus, a high rate capability. After the deposition, the carbon fibers were washed thoroughly with deionized water, and the supernatant were analyzed with UV-vis spectroscopy to assure that there was no residual KMnO4 in the carbon fibers (Supplementary Fig. 4). As shown by SEM, MnO2 started to grow confocally on PCF within the first hour (Fig. 2b), and it continued to grow into nanosheets when the deposition time was prolonged to 2 h (Fig. 2c). The growth of MnO2 on conventional CFs, however, differed drastically. After depositing for 2 h, the surface of CF@MnO2-2h (Fig. 2f) did not change significantly from CF@MnO2-1h (Fig. 2e). Only a thin layer of MnO2 nanosheets was present on the surfaces of both CF@MnO2-1h and CF@MnO2-2h, confirming that the block copolymer-derived PCFs afford a much higher loading of MnO2 than pure PAN-derived CFs. To verify the successful deposition of MnO2 in the mesopores, we compared the transmission electron microscopy (TEM) images of PCF (Fig. 2g) and PCF@MnO2-1h (Fig. 2h). Black spots of MnO2 were uniformly embedded in PCF@MnO2-1h, while they were absent in PCF before loading with MnO2. MnO2 appeared black because Mn has a higher atomic number than carbon does. The PCF mats were prepared on a large scale and ready for use as electrodes without binders or conductive additives (Fig. 2i).
Chemical and physical properties
X-ray photoelectron spectroscopy (XPS), Raman spectroscopy, and high-resolution TEM orthogonally verified the successful loading of MnO2 onto PCF. The XPS spectrum (Supplementary Fig. 5a) of PCF@MnO2-2h showed peaks of C, O, and N corresponding to the carbon fibers, as well as a full set of peaks corresponding to Mn. An examination of the Mn 3s core-level XPS spectrum (Supplementary Fig. 5b) revealed that the separation between the doublet was 4.89 eV, corroborating the valence state of Mn(IV)47. After MnO2 deposition, the Raman spectrum of PCF@MnO2-2h (Supplementary Fig. 6a) showed a group of peaks centered at ~600 cm−1 corresponding to birnessite-phase manganese dioxide (δ-MnO2)48. The birnessite-phase of MnO2 was also proven by the characteristic lattice fringes in the lattice-resolved TEM images (Supplementary Figs. 6b, c). Among the various types of MnO2, δ-MnO2 is one of the most suitable phases for fast charge-discharge because its layered structure allows for rapid ion diffusion49.
The porous structures of carbon fibers changed after loading with MnO2. The pore size distributions of mesopores and micropores were evaluated by nitrogen and carbon dioxide adsorption-desorption isotherms, respectively (Supplementary Fig. 7). PCFs possessed significantly larger numbers of both mesopores and micropores. After depositing MnO2, the micropore volumes of PCFs and CFs steadily decreased at all pore widths, but the peak positions remained unchanged (Fig. 3a, b), suggesting that the micropores were either completely filled or clogged by MnO2. The pore size distributions of PCFs and CFs, however, were different in the mesopore range. PCFs exhibited appreciable decrease in the mesopore volume after depositing MnO2. In addition, the peak position shifted from 11.7 to 10.0 nm after 1 h, and further down to 9.3 nm after 2 h, suggesting that the average thickness of the MnO2 layer inside the pores was ~0.9 nm and ~1.2 nm after depositing for 1 and 2 h, respectively. These thicknesses are desirable for high capacitive performance, as suggested by the Au model in a previous report22. The reduction of mesopore size suggests that the mesopores were only partially filled with MnO2, and therefore they remained accessible to the gas adsorbates and ions. As shown in Supplementary Table 1, the pore volume reduced more in the mesopore range (86.1% reduction after the 2-h deposition) than in the micropore range (66.0% reduction after 2-h deposition). On the contrary, the mesopore volume of CFs, which was two orders of magnitudes lower than that of PCFs, increased after depositing MnO2 (Fig. 3b). The increase in the mesopore volume of CFs is ascribed to the porous structures formed by MnO2 as shown in Fig. 2e, f. The total pore volumes of CF-based electrodes were at least one order of magnitude lower than those of PCF-based electrodes.
The incorporation of MnO2 into PCFs and CFs also altered the surface area (Fig. 3c). The surface area of the PCF mat (574.8 m2 g−1) was more than ten times higher than that of the CF mat (55.31 m2 g−1). Upon loading with MnO2, the surface area of PCFs decreased from 574.8 to 229.5 m2 g−1 for PCF@MnO2-1h, and further down to 187.5 m2 g−1 for PCF@MnO2-2h. In contrast, the surface area of CFs only experienced moderate decreases from 55.31 to 43.35 m2 g−1 for CF@MnO2-1h and to 41.76 m2 g−1 for CF@MnO2-2h.
The higher loadings of MnO2 in PCFs than in CFs is due to the large number of uniform mesopores (Fig. 3d). The total mass loadings (including carbon fibers and MnO2) of PCF, PCF@MnO2-1h, and PCF@MnO2-2h were 3.8 ± 0.1, 6.2 ± 0.3, and 6.8 ± 0.4 mg cm−2, respectively. The error bars ( ± values) are standard deviations determined from at least four independent measurements. MnO2 accounted for 42% and 50% of the total mass of PCF@MnO2-1h and PCF@MnO2-2h, respectively. In contrast, CF-based electrodes showed much smaller mass loadings of 3.9 ± 0.1, 4.2 ± 0.1, and 4.3 ± 0.2 mg cm−2 for CF, CF@MnO2-1h and CF@MnO2-2h, respectively. MnO2 only contributed ~9% of the total mass of CF@MnO2-1h and CF@MnO2-2h. The difference in the mass loading of MnO2 on PCFs and CFs is also apparent in the SEM images (Fig. 2). The comparison shows that the uniform mesopores are indispensable in realizing the high mass loading of MnO2 on the carbon fibers. The abundant mesopores provide large solution-accessible surface areas for loading MnO2 on the PCFs, while micropores can only host a limited amount of MnO2 because the deposition solution can barely access them. The mass of all carbon fibers reduced slightly after loading with MnO2, due to the consumption of carbon by the redox reaction between carbon and KMnO4. Further elongating the deposition time to 3 h showed no appreciable increase in MnO2 loading, confirming that the redox deposition was self-limited.
Ultra-fast electron and ion transport
Considering the high loading of MnO2 and the large number of mesopores for ion transport, we investigated the performance of the PCF-based electrodes for pseudocapacitors. The electron transport and ion diffusion resistivity were analyzed with electrochemical impedance spectroscopy (EIS). The Nyquist plots of PCF, PCF@MnO2-1h and PCF@MnO2-2h (Fig. 4a) exhibited incomplete semicircles followed by linear tails, which resemble the features of mixed kinetic-diffusion-controlled processes and are typical for pseudocapacitive materials50. To obtain the resistances, we fitted the EIS spectra with an equivalent electric circuit (Supplementary Fig. 8). The combined series resistances (Rs) of PCF and PCF@MnO2-1h were 1.0 Ω, and that of PCF@MnO2-2h increased to 1.4 Ω (Fig. 4a inset). The Rs values were comparable to highly conductive carbon-based materials in aqueous electrolytes51,52,53, indicating that MnO2 introduced minimal changes to the electrical resistance of the electrodes despite the high loadings. In addition, the charge-transfer resistances (Rct, the semicircles in Fig. 4a inset) of PCF, PCF@MnO2-1h and PCF@MnO2-2h are 0.74, 0.86 and 1.30 Ω, respectively. The small resistances suggest efficient electron transfer associated with the redox reaction of MnO2. The augmentation of charge-transfer resistance in PCF@MnO2-2h is mainly due to the increased thickness of MnO2 deposited in the mesopores (evidenced by the reduction in mesopore-width shown in Fig. 3d). The increased thickness elongates the electron transport distance in MnO2 and therefore obstructs electron transfer at the MnO2/electrolyte interface, because MnO2 is a poor electron conductor (10−5~10−6 S cm−1). The small Rs and Rct are key attributes of the block copolymer-based carbon fiber electrodes because 1) unlike discrete carbon particles or graphene flakes, the carbon fibers offer continuous expressways for electron conduction, and 2) the block copolymers endow the carbon fibers with high surface areas to load with an ultrathin layer of δ-MnO2, which mitigates the insulating problem and facilitates the electron transport.
In addition to the efficient electron transport, the block copolymer-derived PCF electrodes exhibited ultra-fast ion diffusion kinetics, as featured by their ultra-small diffusion resistances (σ). The values of σ were extracted from the slopes of the linear fitting lines of the real part of impedance (Z’) versus the reciprocal of the square root of frequency (ω−0.5) (Fig. 4b). PCFs displayed the smallest σ of 0.64 Ω s−0.5, followed by PCF@MnO2-1h (1.18 Ω s−0.5) and PCF@MnO2-2h (1.68 Ω s−0.5). The slight increase in σ is in accordance with the fact that the pseudocapacitive reactions are slower than the adsorption-desorption of ions pertaining to the electrical double layer capacitive processes, as well as that the mesopore size is reduced. Despite the increase, the σ values of our PCF-based electrodes were remarkably smaller than other MnO2-based materials (Fig. 4c). Notably, the σ value of PCF@MnO2-2h was even lower than that of CF (Fig. 4c and Supplementary Fig. 9), a mostly electrical double layer capacitive (EDLC) material that has fast ion diffusion kinetics. In addition, the σ value of PCF@MnO2-2h ( < 2 Ω s−0.5) is ~3.5 times lower than that of CF@MnO2-2h (~7 Ω s−0.5), highlighting the critical role of the uniform distributed, randomly oriented, and interconnected mesopores in accelerating electrolyte infiltration and ion diffusion in block copolymer-derived PCFs.
With continuous electron conduction and ultra-low ion diffusion resistivity, PCF@MnO2-2h exhibited ultra-fast charge and discharge kinetics. The cyclic voltammograms (CVs) of PCF@MnO2-2h were nearly rectangular (Fig. 5a), reflecting the rapid electron and ion transport in the electrode54. The current density of a supercapacitor, i, scales with the scan rate, v, following the relationship of i = kvb. The power-law exponent, b, is an important metric to evaluate the charge-storage kinetics, and b = 1 for an ideal supercapacitor. By plotting the logarithm of the absolute cathodic current densities at 0.2 V against the logarithm of scan rates (Fig. 5b), the b-value was calculated to be 0.93 in the scan-rate range of 10-100 mV s−1, approaching that of an ideal capacitor (b = 1) and suggesting the ultra-fast charge-storage kinetics. Outstandingly, the b value decreases only slightly to 0.91 in the range of 10–1000 mV s−1, unambiguously confirming its fast charge-storage kinetics.
We further decoupled the capacitances from fast-kinetic processes and slow-kinetic processes. The decoupling is based on the different contributions of fast and slow kinetics processes in the current density of a CV curve (see Supplementary Methods for details). Briefly, the current density at a fixed potential and a scan rate, i is composed of two terms associated with the scan rate, v:
where k1 and k2 are constants. The first term k1v equals the current density contributed from fast-kinetic processes and the second term k2v0.5 is the current density associated with slow-kinetic (or diffusion-controlled) processes. Dividing v0.5 on both sides of Equation (1) gives:
Equation (2) shows that iv0.5 and v0.5 are expected to have a linear relationship, with k1 and k2 being the slope and the y-intercept, respectively. Repeating the above step at other scan rates reveals the current density contribution across the potential window and outlines the contribution from the fast-kinetic and slow-kinetic processes. Figure 5c shows an example of the decoupling of a CV at 100 mV s−1. The capacitive contribution from the fast-kinetic processes (yellow region) clearly dominates that of the slow-kinetic processes (blue region) at all scan rates (Fig. 5c–d, Supplementary Fig. 10). The slow-kinetic capacitance decreased with the increasing scan rate. Importantly, the electric double layer capacitance (Cdl) contributed only a small fraction in the fast-kinetics region (Fig. 5d, gray dashed line), indicating that the majority of the pseudocapacitance of PCF@MnO2-2h is not charge-transfer-limited or diffusion-controlled. The fast kinetics makes PCF@MnO2 a desirable pseudocapacitive electrode for rapid charge storage and release.
We measured the electrochemical capacitive performance of our carbon fiber electrodes. Among the PCF-based electrodes, PCF@MnO2-2h displayed the highest areal capacitance, as shown by the CVs (Fig. 6a) and the galvanostatic charge-discharge (GCD) profiles (Fig. 6b). The negligible deviation of the CVs from the rectangular shape and the isosceles triangular GCD profiles at high 10 mA cm−2 echoed the fast charge-storage kinetics of PCF@MnO2. A radar chart (Fig. 6c) summarizes the six figure-of-merits of a pseudocapacitor electrode, i.e., mass loading, gravimetric capacitance normalized to the mass of MnO2, gravimetric capacitance normalized to the mass of electrode, areal capacitance normalized to geometric surface area, areal capacitance normalized to BET surface area, and rate capability. Due to the lower mass loading of PCF@MnO2-1h than that of PCF@MnO2-2h, the former achieved higher values in gravimetric capacitance and rate capability. Remarkably, the gravimetric capacitance of PCF@MnO2-1h at 10 mV s−1 reached 1148 F g−1 of MnO2. This value is ~84% of the theoretical gravimetric capacitance of MnO2 (1367 F g−1) within a potential window of 0.8 V, even slightly higher than those on the model supports of mesoporous Au22,23 and dendritic Ni26, suggesting almost all the MnO2 loaded on PCFs was accessible to the ions and contributed to the high capacitance. PCF@MnO2-2h displayed the highest areal capacitance owing to its highest mass loading. PCF exhibited the best rate capability because it charges/discharges mostly via electrical double layers. Full comparison of the gravimetric, areal, and volumetric capacitances of PCF-based and CF-based electrodes at various scan rates are summarized in Supplementary Figs 11 and 12. Markedly, the gravimetric capacitance and geometric areal capacitance of PCF@MnO2-2h outperformed the previously-reported MnO2 electrodes at comparable mass loadings under similar testing conditions (Fig. 6d and Supplementary Table 2). Ideally, with fast electron and ion transport at high mass loadings, both the areal and gravimetric capacitances are expected to be high. However, most reported MnO2 electrodes have poor areal and/or gravimetric capacitances. In contrast, our PCF-supported MnO2 electrodes have both high areal and gravimetric capacitances. PCF@MnO2-2h was also highly stable, retaining more than 98% of the initial capacitance after 5000 consecutive charge-discharge cycles (Supplementary Fig. 13).
The Ragone plot (Supplementary Fig. 14) compares the specific energy and power densities of PCF@MnO2 with those of the MnO2 supported on graphene, a star material for supercapacitor electrodes. With a high gravimetric power density of 23.2 kW kg−1 and a high gravimetric energy density of 10.3 Wh kg−1 in the tested range of scan rates, PCF@MnO2-2h outperformed the various graphene- and CF-supported MnO2 electrodes in symmetric pseudocapacitors. The superior capacitive performance signifies that our PCF-supported MnO2 electrodes have realized both high mass loadings and ultrafast charge transport kinetics.
The judiciously designed comparison between our PCFs and conventional CFs proves that PCFs with uniform mesopores are superior carbon supports for addressing the two long-lasting challenges of pseudocapacitors: high mass loading and fast charge transport. Utilizing the concept of block copolymer self-assembly and microphase separation, PCFs provide abundant mesopores with a large surface area for high mass loadings of ultrathin (<2 nm) pseudocapactive materials. On the one hand, the ultrathin pseudocapactive material, along with the continuous fibrous carbon network, renders the composite electrode fast electron transport. On the other hand, the partially filled mesopores provide continuous and wide-open channels for effective ion transport with little diffusion resistance, even at high mass loadings approaching 7 mg cm−2. The PCF@MnO2 electrodes show outstanding and balanced gravimetric capacitance, areal capacitance, and rate capability, which outperform other MnO2-based pseudocapacitive electrodes at comparable mass loadings and testing conditions. Future investigations on the interplays among the polymer molecular weight, mesopore size, mass loading of MnO2, ion diffusion resistivity and the use of ionic liquid electrolytes55 are expected to further optimize the capacitive performance of PCF@MnO2 and enhance the energy density of the supercapacitors.
This work signifies the great potential of leveraging the disparate and innovative concept of block copolymer microphase separation to design and fabricate mesoporous carbon fiber supports. We emphasize that the highly uniform mesopores are crucial for the high loading of guest materials and the efficient transport of ions. The block copolymer-derived PCFs revolutionize the porous carbon supports and are adaptable to a broad range of electrochemical applications including batteries, fuel cells, catalyst supports, and capacitive desalination devices.
Synthesis of porous carbon fiber mats
Porous carbon fiber (PCF) mats were derived from poly(acrylonitrile-block-methylmethacrylate) (PAN-b-PMMA) block copolymer. Briefly, PAN-b-PMMA (Mn = 110-b-60 kDa, polydispersity = 1.14) was synthesized via reversible addition-fragmentation chain-transfer polymerization56 and electrospun into a polymer fiber mat. The polymer fiber mat was cut into small stripes (e.g., 10 cm × 2 cm), loaded into a tube furnace (Thermo-Fisher Scientific, Model STF55433C-1), and then heated at 280 °C for 8 h (ramp rate: 1 °C min−1) in air. The heating process induced the microphase separation of PAN and PMMA, and it triggered the crosslinking and cyclization of PAN. The resulting brown mats were further heated at 1200 °C for 1 h (ramp rate: 10 °C min−1) under a nitrogen atmosphere. Afterwards, the tube furnace was cooled down to room temperature and PCF mats were obtained. The preparation of CF was similar except that PAN was used instead of PAN-b-PMMA.
Deposition of Manganese Dioxide
Manganese dioxide (MnO2) was deposited onto the PCF mats via a solution-based self-limiting redox reaction with potassium permanganate (KMnO4),
First, 0.032 g of KMnO4 powder was dissolved in 20 mL of deionized water and used as the deposition solution (KMnO4, 10 mM). The solution was then heated to 80 °C under ambient pressure. Approximately 10 mg of PCF mats were soaked in the solution for 1–2 h under gentle stirring. After the reaction, the KMnO4 solution was drained and the remaining carbon fiber mats were thoroughly washed with deionized water five times, followed by drying in a vacuum oven at 60 °C for 8 h. The resulting carbon fiber mats are designated as PCF@MnO2-1h and PCF@MnO2-2h based on the reaction times of 1 h and 2 h, respectively.
The mass loading of MnO2 was determined by calculating the mass difference between the PCF mats before and after the reaction (see Supporting Information for detailed calculations). The areal mass loadings of MnO2 in PCF@MnO2-1h and PCF@MnO2-2h were 2.6 ± 0.2 and 3.4 ± 0.4 mg cm−2, respectively. The total mass loadings (including PCF and MnO2) of PCF@MnO2-1h and PCF@MnO2-2h were 6.2 ± 0.3 and 6.8 ± 0.4 mg cm−2, respectively. The average thickness of all PCF, PCF@MnO2-1h and PCF@MnO2-2h mats was ~200 μm. Thus, the volumetric mass densities of PCF@MnO2-1h and PCF@MnO2-2h were 0.31 ± 0.02 and 0.34 ± 0.02 g cm−3, respectively. The standard deviations were based on at least three batches of carbon fiber based electrodes.
Electrochemical deposition was also adopted to prepare PCF@MnO2 electrodes with high mass loadings. The electrodeposition solution contained 0.1 M manganese acetate and 0.5 M lithium chloride (a supporting electrolyte) in deionized water. A piece of PCF carbon fiber mat, a piece of nickel foam, and an Ag/AgCl wire in saturated KCl aqueous solution were used as the working electrode, the counter electrode, and the reference electrode, respectively. The electrodes were connected to an electrochemical workstation (PARSTATS 4000+, Princeton Applied Research, Ametek Inc.) and scanned between 0 and 1.0 V vs. Ag/AgCl at a scan rate of 0.01 mV s−1 for 15 cycles. The mass loading of the electrodeposited MnO2 on the PCF was 4.2 mg cm−2. The total mass loading (including PCF and MnO2) from electrodeposition was ~8.0 mg cm−2.
The carbon fibers were characterized using scanning electron microscopy (SEM, LEO Zeiss 1550, acceleration voltage: 2 kV) and high-resolution transmission electron microscopy (HRTEM, FEI TITAN 300, acceleration voltage: 300 kV). The physisorption isotherms were measured with a pore analyzer (3Flex Pore Analyzer, Micromeritics Instrument Corp.) using nitrogen (for mesopores) and carbon dioxide (for micropores). Prior to the sorption tests, all electrodes were heated at 90 °C for 60 min and then at 200 °C for 900 min in N2 to desorb any moisture and hydrocarbons. The ramping rate of both heating processes was 10 °C min−1. The surface areas were calculated using the Brunauer-Emmett-Teller (BET) method, and the pore size distributions were obtained by the density functional theory. X-ray photoelectron spectroscopy (XPS) spectra were acquired using monochromatic Al Kα X-ray source (1486.6 eV) with a 200 µm X-ray beam at an incident angle of 45°. All binding energies were referenced to adventitious C 1 s at 284.8 eV. Chemical states of elements were assigned based on the National Institute of Standards and Technology (NIST) XPS Database. Raman spectra were recorded by a Raman spectrometer (WITec alpha 500) coupled with a confocal Raman microscope using a laser excitation wavelength of 633 nm. UV-vis spectra were measured by an Agilent Cary 60 UV-vis spectrometer. Small angle X-ray scattering (SAXS) spectra were collected by a Bruker N8 Horizon instrument with Cu Kα radiation (λ = 1.54 Å) at a current of 1 mA and a generator voltage of 50 kV.
The electrochemical performance was evaluated in a symmetric two-electrode configuration in an aqueous electrolyte of 6 M KOH. For consistency, carbon fiber mats were sandwiched between two pieces of nickel foams (EQ-bcnf-80 μm, MTI corporation). Cyclic voltammograms were collected within a potential window of 0–0.8 V at various scan rates of 10–1000 mV s−1. Galvanostatic charge and discharge (GCD) were performed within the same potential window (0–0.8 V). Electrochemical impedance spectroscopy was conducted at open circuit potentials with frequencies between 0.1 Hz and 100 kHz with a perturbation of 5 mV. The CVs and EIS were recorded using a PARSTATS 4000 + electrochemical workstation (Princeton Applied Research, Ametek Inc.). The GCD curves were acquired from a charge-discharge cycler (Model 580, Scribner Associates Inc.).
Data supporting the findings of this study are available in this paper and in the Supplementary Information or are available from the corresponding author upon reasonable request.
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This material is based upon work supported by the Air Force Office of Scientific Research under award number FA9550-17-1-0112 through the Young Investigator Program (YIP). Guoliang Liu acknowledges the American Chemical Society Petroleum Research Foundation for the Doctoral New Investigator (DNI) award. The authors acknowledge the use of electron microscopes in the Virginia Tech Institute for Critical Technology and Applied Science (ICTAS), and Dr. Xu Feng for assistance in the XPS analysis at the Surface Analysis Laboratory of Virginia Tech. The XPS is supported by the National Science Foundation under Grant No. CHE-1531834.
The authors declare no competing interests.
Journal peer review information Nature Communications thanks Christopher Arges and the other anonymous reviewers for their contribution to the peer review of this work. Peer reviewer reports are available.
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Liu, T., Zhou, Z., Guo, Y. et al. Block copolymer derived uniform mesopores enable ultrafast electron and ion transport at high mass loadings. Nat Commun 10, 675 (2019). https://doi.org/10.1038/s41467-019-08644-w
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