1School of Materials and Chemistry, University of Shanghai for Science and Technology, Shanghai 200093, China.
2Department of Materials Science, Fudan University, Shanghai 200433, China.
#Authors contributed equally.
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The lithium-sulfur battery is currently considered to be a promising candidate for next-generation energy storage devices. However, its commercial application is severely restricted by rapid capacity decay mainly arising from unavoidable dissolution of intermediate lithium polysulfide of the S-based cathodes. Herein, multifunctional stripped grapheme-carbon nanotubes (SG-CNT) with 1D/2D interwoven and hierarchical pore structure as a promising host to stabilize S was constructed by cheaper raw materials and a facile strategy. Based on comprehensive analysis, the interwoven network and hierarchical pores along with abundant oxidative functional groups in matrix provided large contact area with S, short transport pathway for electrons/Li-ions, sufficient space to accommodate volumetric change, and superior confinement ability for S/polysulfides, thus resulting in effectively stabilizing the S cathode with high S loading and increasing its utilization. Therefore, the S@SG-CNT cathodes exhibited a high reversible capacity of 1227 mAh g-1 at 0.1 A g-1, excellent cyclability with a capacity of
Graphene, carbon, hierarchical pores, cathode, Li-S battery
The lithium-sulfur (Li-S) batteries have attracted enthusiastic interest as powerful energy storage systems owing to their overwhelmingly high theoretical energy density (2580 Wh kg-1) and gravimetric capacity (1672 mAh g-1). The most incomparable advantages of S are that it is naturally low cost, abundant, and environmentally friendly, making the Li-S battery one of most hopeful candidates of next-generation battery technology[1-4]. Unfortunately, the Li-S battery still presents fast capacity fading, low overall capacity, and high self-discharge, which are attributed to: (1) low S content and large volume change during the lithiation/delithiation process; (2) very poor electrical conductivity induced by insulating of S; and (3) internal “shuttle reaction” arising from the dissolution of lithium polysulfide (LPS) intermediates (Li2Sx, 4 ≤ x ≤ 8) into organic electrolytes[5-7].
To overcome the low utilization and low loading, encapsulating S into carbonaceous materials with pore structure has been considered as an effective tactic in the past few decades. In this case, architecting pore structure is a key for the S and Li-S battery because it directly determines the loading amount and subsequent confinement effect. It is well known that microporous (the pore size < 2 nm) can accommodate S and prevent the formation of LPS; however, it is easy to block solid products and eventually limit the penetration of electrolyte during cycling. Mesopores (2-50 nm) have been considered as a hopeful type; however, they cannot simultaneously achieve abundant accommodation of S, effective alleviation of soluble LPS. And fast Li-ion transport in the electrolytes. Macropores (> 50 nm) attain the high loading of S owing to its large pore size, but they are not conducive to retarding the shuttle of LPS[9-11]. To overcome these single-sized porous limitations in carbon materials, a hierarchical pore structure, which combines the strengths of the three pore sizes synergistically, could be used. In addition to the size distribution of pores, the existence of abundant pores (especially the large-size pores) in the carbonaceous materials also impacts on the original matrix structure and its conductivity, which can further influence the long-cycling performance. It is worth noting that a three dimensional (3D) cross-linked network in the carbonaceous materials, compared with 1D and 2D carbon-based materials, can not only ensure structure stability against deformation but also facilitate the electron/ion transport, which can in turn achieve mass transport and fast electrode kinetics. Consequently, a hierarchical pore structure and conductive microstructure of carbon materials is desired for Li-S batteries.
More importantly, besides physically confining S in porous structures, the chemical interaction between the functional carbon matrix and S also exerts a positive impression on the Li-S battery’s performance. As described in the relevant literature, the oxidative functional groups (OFG) on the surface of the matrix show strong effects on the polysulfide anions and can trap LPS into the organic electrolyte during the lithiation process. For instance, porous structures with a large amount of OFG can improve the capacity retention of S cathodes while limiting the diffusion of LPS into electrolyte, which might be attributed to the strong binding effects between the LPS and the OFG of the active matrix. Similarly, Ji et al. reported that the abundant OFG on the surface of the graphene oxide could immobilize S, therefore improving the electrochemical performance. Recently, constructing a unique microstructure and introducing polar materials (such as metal oxides/selenides/sulfides and metal atoms) can display a more compact adsorption of LPS than a carbon-based matrix, which can further enhance cycling performance for Li-S batteries[17-21]. However, these methods are very complicated. Motivated by the above discussions, using a facile strategy to design a matrix containing hierarchical pores and stable microstructure together with abundant OFG is favorable for Li-S batteries, with the aim that it will exhibit high reversibility and ultra-long cyclic stability of S cathodes.
In this study, multifunctional 3D stripped grapheme-carbon nanotubes (denoted as SG-CNT) with hierarchical structure were firstly prepared by a facile oxidation-reduction method, and subsequently an infiltration method was employed to load S to fabricate S@SG-CNT composites at high temperature for Li-S battery cathodes. In the S@SG-CNT composites, the SG-CNT host possesses 1D/2D intrinsic interwoven carbonous matrix [1D CNT skeleton and 2D stripped graphene (G) sheets with covalent C-C bonds], micro-meso-macro hierarchical pores, and abundant oxidative functional groups, providing solid contact with S, short transport pathway for both electrons and Li-ions, sufficient room to accommodate volumetric change, and superior retarding ability for the shuttle of LPS. The S@SG-CNT cathodes containing more than 64 wt.% S present high reversible specific capacity and excellent rate cycling stability, especially a low capacity decay rate of less than 0.01% per cycle within 2000 cycles at a higher current rate of 2.0 A g-1. The systematic results can provide a new insight into the 1D/2D structural design for matrix host for Li-S batteries.
Synthesis of S@SG-CNT: Firstly, the SG-CNT was synthesized from multi-walled CNT by a modified Hummer’s method. Before transferring the oxidized CNT to the hydrothermal reactor, the solution was ultrasonicated for half an hour. After that, this solution was placed into a Teflon-lined stainless-steel autoclave for hydrothermal at 200 °C for 48 h. Finally, the as-prepared SG-CNT hydrogel was freeze-dried. Then, the S@SG-CNT was prepared by infiltration of the sublimed S powder into SG-CNT in evacuated quartz capsule (mSG-CNT:mS = 3:7) at 700 °C for 6 h. From that, the S@SG-CNT was obtained after cooling down to room temperature. For comparisons, S@CNT and S@O-CNT were prepared by carbonizing of merging pure CNT and O-CNT with sublimed S, respectively.
Physical characterizations: SEM images were obtained by using a FEI Nova SEM 230 (form Oxford Instruments, named INCA X-Max 80). Deep morphologies and microstructure were characterized by TEM at 200 kV (JEOL Ltd. from Japan). The XRD patterns were recorded on X-ray diffractometer (Rigaku D/MAX-2200/PC) with a Cu Kα radiation at 40 kV and 20 mA. Raman spectra were obtained by a Senterra R200-L. The surface properties were analyzed by XPS (Kratos Axis Ultra DLD). BET and porosity of the as-synthesized sample were carried out using a N2 sorption instrument (Micromeritics, ASAP2020). To confirm the S content in S@CNT, S@O-CNT, and S@SG-CNT, thermogravimetric analysis (TGA) was performed with a heating rate of 10 °C/min (a Netzsch STA 449 F1, Germany) and high-purity N2 as the purge gas.
Electrochemical measurements: The electrochemical performance was tested using 2032 half-cell. The composite was mixed with carbon black and polyvinylidene fluoride in a weight ratio of 85:5:10, with N-methylpyrrolidone solvent as a dispersant. The as-prepared slurry was coated onto an Al foil. After that, the electrodes were punched into circle discs. The battery was assembled in a glovebox (MBRAUN). Before being transferred to the glovebox, the electrodes were further dried in a vacuum at 60 °C for 24 h. Li metal was used as a counter; Celgard 3501 (Celgard, LLC Corp., USA) was used as a separator; and 1.0 M LiTFSI was dissolved in a mixture of 1,3 DOL/1,2 DME (1:1 v/v) with 1.0 % wt. LiNO3 additive was applied as the electrolyte. The electrolyte/S ratios were 11 and 8 μL mg-1 for cathodes with S loading of ~2.4 mg cm-2 and higher S loadings (4.1, 5.3, and 6.6 mg cm-2), respectively. Cycling performances were tested in the potential range of 1.5-3.0 V on a LAND CT2001A battery test system (Wuhan Jinnuo Electronics, Ltd.). Cyclic voltammetry (CV) was performed at a scan rate of 0.1 mV s-1 (Gamry Co., Reference 3000, USA). Before electrochemical impedance spectroscopy (EIS) tests, the cell was cycled to the target cycle number at
Figure 1 displays the schematic diagram of the preparation processes of ultrafine S particles confined in the CNT, oxidized CNT (O-CNT), and stripped-G CNT (SG-CNT), respectively. First, O-CNT was prepared via a facile oxidation method, which can easily introduce abundant OFG and more defects on the outer walls of CNT. After hydrothermal reaction, a black hydrogel can be facilely obtained via a self-assembly condensation reaction. Meanwhile, the C-C bonds around the defects and disorder of the outer CNT walls prefer to break each other, and then the outer walls of CNT are automatically stripped, becoming 2D G sheets. After that, the 2D G sheets can enwrap and string the inner 1D CNT to become a 1D/2D intrinsically coupled structure (SG-CNT), and the exposed edges of the broken CNT have a great tendency to produce plentiful oxidative functional groups. Following freeze-drying, we can achieve a 3D SG-CNT sponge with more porous structure, which can facilitate the absorption of S vapor by the strong capillary effect during the following high-temperature infiltration. Upon vaporization, S vapor can easily permeate into the empty volume of the SG-CNT matrix by a large driving force at high temperature. To investigate the influence of the unique structure of SG-CNT on the electrochemical performances, the S@SG-CNT, S@CNT, and S@O-CNT composites were prepared by combination of merging the CNT and O-CNT with sublimed S under the same condition, respectively. In contrast to the S@CNT and S@O-CNT composites, it was hypothesized that S@SG-CNT would present excellent electrochemical performance owing to the cross-linked skeletons and pore structure promoting interactions between ultrafine S and the SG-CNT matrix.
Figure 1. Schematic diagrams of the preparation processes of S@CNT, S@O-CNT, and S@SG-CNT, respectively.
The morphologies of the three matrices were elucidated by SEM and TEM. At the suspended solution stage, the O-CNT with oxygen-functional groups can uniformly disperse as compared with the pristine CNT
Figure 2. (A-C) SEM images of (A) CNT, (B) O-CNT, and (C) SG-CNT; (D-F) TEM images of (D) CNT, (E) O-CNT, and (F) SG-CNT; and (G) schematics of oxygen functional groups in CNT (left), O-CNT (middle), and SG-CNT (right).
XPS measurements were used to investigate the chemical compositions as well as the oxidation state of the elements. As depicted in Figure 2F and Supplementary Figure 3, the CNT, O-CNT, and SG-CNT samples are all mainly composed of O and C elements, while the atomic ratio of O/C in the O-CNT and SG-CNT samples decrease from 0.288 to 0.154 [Figure 2F and Supplementary Table 1], implying that the OFG were assembled under high temperature (200 °C) and pressure during the hydrothermal process. The O 1s XPS spectra of the O-CNT and SG-CNT in Figure 2F and Supplementary Figure 4 exhibit four peaks at 534.3, 533.2, 532.0, and 531.2 eV, which are assigned to the carboxylic, epoxide, hydroxyl, and carbonyl groups, respectively. Interestingly, the main O-containing functional groups in the SG-CNT change to epoxide groups (occupying 7.73 at.%; see Figure 2F and Supplementary Table 2) accompanied by decrease of the carboxylic (1.12 at.%) and hydroxyl (3.69 at.%) groups after hydrothermal reaction. Such dynamic change of the O-containing functional groups in the carbon framework of SG-CNT shows a stable covalent linkage between carbon material. For instance, the OFG can improve the wettability in the inert surface area and expose more active sites to absorb S. Besides, all O-containing functional groups readily trap S species. Moreover, the hydroxyl groups, which were abundant after high-temperature vapor infiltration, show stronger chemical interaction to the polysulfide anions than do the epoxide groups[26,28]. This is due to the fact that abundant hydroxyl groups
The S@CNT, S@O-CNT, and S@SG-CNT composites were obtained with high-temperature vapor infiltration method. The S contents were measured by TGA [Figure 3A], which indicated that the S contents in S@CNT, S@O-CNT, and S@SG-CNT are 63.75%, 64.53%, and 64.36%, respectively. The equal S mass content in these three composites is convenient to compare the battery performance without concerning the variation of the S loading.
Figure 3. (A) TGA patterns of S@CNT, S@O-CNT, and S@SG-CNT; (B) XRD and (C) pore size distribution of CNT, O-CNT, and SG-CNT; (D) N2 adsorption isotherms of SG-CNT and S@SG-CNT; (E) high-resolution XPS spectra of S 2p of three composites; (F) SEM images of S@SG-CNT; (G) TEM images of S@SG-CNT; and (H-K) STEM image of the representative S@SG-CNT (H) and corresponding C (I), O (J), and S (K) element mapping.
The phase composition of the S@CNT, S@O-CNT, and S@SG-CNT samples were measured. The XRD peaks of crystalline S are observed in Figure 3B for S@CNT and S@O-CNT, while the peak intensity of S is drastically weakened for S@SG-CNT sample, which suggests that the ultrafine S nanoparticles are evenly distributed in the nanoscale pores and exclusively confined between the carbon layers in the SG-CNT host. The existence of a strong intimate interplay between S and SG-CNT host led to a relatively poor crystallinity compared to the S@CNT and S@O-CNT. This was further evidenced by Raman analysis
The pore size distribution and specific surface area (SSA) of three S-implanted composites and corresponding matrix were evaluated by N2 adsorption tests. As shown in Figure 3C, a hierarchical structure with micro-meso-macro pore size distribution was observed in the S@SG-CNT matrix. Besides, the SSA and the pore volume of the S@CNT, S@O-CNT, and S@SG-CNT composites in Figure 3D and Figure 2F and Supplementary Figure 6 are much smaller than their corresponding matrix. For instance, the pore volume and SSA of SG-CNT is 1.274 cm3 g-1 and 310.9 m2 g-1, while the corresponding values decreased to 0.458 cm3 g-1 and
To further elucidate the interaction between matrix and S, the chemical environments of three composites were also elucidated by XPS analysis. As shown in Figure 2F and Supplementary Figure 7 and Figure 2F and Supplementary Table 3, the O elements could only be detected for S@SG-CNT and could hardly be found in S@O-CNT, which indicates that most OFG were removed from the O-CNT after hydrothermal process, while the robust C-O bonds could be maintained in SG-CNT. We therefore believe that the hydrothermal process helps oxygen-containing functional groups anchor on carbon matrix with strong chemical bonds. As shown in Figure 2F and Supplementary Figure 8, the deconvolution plot of the C 1s XPS spectra for S@SG-CNT shows four peaks at 289.0, 286.7, 285.6, and 284.7 eV, which correspond to O-C=O, C=O, C-O/C-S, and C=C/C-C bonds, respectively. The occurrence of C-S bonds suggests that S atoms were doped in SG-CNT and formed a robust bond during the high-temperature treatment. The O 1s XPS spectrum for the S@SG-CNT
The morphology evolution of S@CNT, S@O-CNT, and S@SG-CNT composites were also investigated. As shown in Figure 3F and Figure 2F and Supplementary Figure 11, there was no obvious structure change for the three composites after the S impregnation. In comparison, the 1D/2D interwoven structure was observed in S@SG-CNT, while it vanished in S@CNT and S@O-CNT. Notably, bulk S particles [Figure 2F and Supplementary Figure 12] could not be clearly detected in the SEM image of S@SG-CNT, which may be attributed to the fact that the S molecules were uniformly and ultra-finely confined for the S@SG-CNT composite. This above phenomenon could also be proved by the TEM image of S@SG-CNT. In contrast with the TEM images of S@CNT and S@O-CNT in Figure 2F and Supplementary Figure 13, the 3D CNT-bridged G structure can be recognized in S@SG-CNT, which can reach excellent properties by keeping the matrix structure stability during the cycling process and improving the electrical conductivity. Figure 3G shows the S could encapsulate in carbon nanotubes at high temperature and pressure. The adjacent fringe spacing is around 0.34 and 0.38 nm, corresponding to the (026) and (038) plane of S, respectively, implying that a robust intimate contact existed between S and the SG-CNT matrix, which complies with the XPS results. The EDS mapping of S@SG-CNT was used to confirm the distribution of elements. Figure 3H-K shows that the three elements (C, O, and S) in S@SG-CNT were uniformly distributed in the large region.
To demonstrate the role of unique structural benefits of the SG-CNT sponge with 3D cross-linked hierarchical pore structure and the interaction of S-O play in enhancing cathode performance of the Li-S battery, the electrochemical properties of the serial materials were measured and compared. Figure 4A depicts the initial five CV of the S@SG-CNT electrode under a voltage range of 1.5-3.0 V (vs. Li/Li+). Three reduction peaks (~2.35, ~2.0, and ~1.7 V) were observed in cathodic scan, which were ascribed to the reduction of high-order polysulfides (Li2Sx, 4 ≤ x ≤ 8) to low-order polysulfides (such as Li2S4, Li2S2, and
Figure 4. Electrochemical performance of the electrode based on the sulfur mass: (A) Cyclic voltammetry curves of S@SG-CNT electrodes at a scan rate of 0.1 mV s-1; (B) initial three discharge/charge profiles of S@SG-CNT cathode at a current density of 0.1 A g-1; (C) rate-cycle performance; (D) the second charge/discharge curves of the S@SG-CNT at 0.1, 0.2, 0.5, 1.0, 2.0, and 5.0 A g-1, respectively; (E) cycling performance at 200 mA g-1; (F) the 2nd, 100th, 200th, and 500th charge/discharge curves of the S@SG-CNT at 0.2 A g-1, respectively; (G) long-term cycling performance; and (H) long cycling life of the S@SG-CNT with four different mass loading of S at 2000 mA g-1.
Figure 4B exhibits the initial three discharge/charge profiles of S@SG-CNT cathodes under 0.1 A g-1. The three discharge plateaus (~2.3, ~2.0, and ~1.7 V) and one charge plateau (~2.35 V) were displayed for the S@SG-CNT composites in the first cycle, which is accordance with the above observation of CV. The S@SG-CNT delivers an ultra-high discharge/charge capacity of 1647.5/1321.1 mAh g−1, which can give a high Coulombic efficiency (CE) of 80.2% in the first cycle. Upon cycling, the plateau at ~1.7 V disappeared, consistent with the CV results. Meanwhile, a high discharge capacity was sustained at 1226.6 mAh g-1 in the second cycle, and the CE exceeded to 95%. In comparison, the pristine S, S@CNT, and S@O-CNT cathodes only displayed discharge capacities (1130, 1220, and 1346 mAh g-1, respectively) in the first cycle and corresponding CE (65.4%, 79.3%, and 71.5%, respectively) [Figure 2F and Supplementary Figure 15]. The low capacities and CE were due to the large capacity loss of the pristine S, S@CNT, and S@O-CNT cathodes, caused by the dissolved polysulfides due to the unsuitable architectures of the S@CNT and S@O-CNT composites. Thus, it is safe to say that the excellent battery performance and the high initial CE of the S@SG-CNT composites are the result of the unique 1D/2D interwoven structure and the strong chemical interaction of S-O-containing functional groups involving the SG-CNT matrix.
In addition, the S@SG-CNT cathode displayed excellent capability under various current densities. As shown in Figure 4C, high reversible specific capacities of 1201, 991, 860, and 772 mAh g-1 for the S@SG-CNT cathodes could be obtained at 0.1, 0.2, 0.5, and 1.0 A g-1, respectively. More importantly, excellent discharge capacities of 720 and 655 mAh g-1 could still be achieved for the S@SG-CNT electrodes even up to ultra-high C-rates of 2.0 and 5.0 A g-1, respectively. Following that, when the current density returned to
To further evaluate the structural of the S@SG-CNT composite structure, the long cycling performance of the three composites were investigated. As shown in Figure 4E, the S@SG-CNT composites exhibited a very high reversible capacity of 1309.5 mAh g-1 at 0.2 A g-1 and then reached 880 mAh g-1 at around the 100th cycle after undergoing the initial activation procedure. Even up to 500 cycles, the reversible capacity of the S@SG-CNT still maintained 773 mAh g-1, yielding a capacity retention of around 87.8%. Upon cycling, the corresponding CE tended to increase to 100% after 50 cycles, reflecting the excellent reversible capacity and low influence of the electrochemical shuttle effect. In contrast with the S@SG-CNT composites, the S@CNT and S@O-CNT cathodes showed very low discharge capacities of 281 and 538 mAh g-1 under the same current density (200 mA g-1) after 500 cycles, much lower than that of the S@SG-CNT composites. In addition, the S@SG-CNT material also displayed excellent cycling performance at low E/S ratio (see Figure 2F and Supplementary Figure 17). The S@SG-CNT composites exhibited better performance than some previous works (see Table 1)[17-21,43-49]. In addition, the typical reproducible charge/discharge curves in Figure 4F imply the highly reversible stability of the S@SG-CNT composites. In addition, S@SG-CNT also showed excellent cyclability at a high current density. As shown in Figure 4G, the S@SG-CNT composites displayed an initial capacity of 743.1 mAh g-1 and maintained 551.2 mAh g-1 with CE close to 100% even after 2000 cycles, while the S@CNT and S@O-CNT cathodes only showed 184 and 318 mAh g-1 under the same current density (2000 mA g-1) after 1000 cycles, implying that S@SG-CNT exhibits excellent rate performance. The improved rate capabilities of S@SG-CNT is attribute to the collaborative effects including the good electrical conductivity, which emanate from the unique “one in two” structure with CNT-bridged stripped G interwoven and the effective inhibition of “shuttle effect” due to the hierarchical pores and the strong S-O interaction via OFG in the smart 3D SG-CNT building blocks. To reveal the practical application of the S@SG-CNT composite, the electrochemical properties of the electrodes with high mass loading of S were investigated. Figure 4H shows the long cycling life of the S@SG-CNT composite with four different mass loadings of S (2.6, 4.1, 5.3, and 6.6 mg cm-2) at 2.0 A g-1. As shown in Figure 4H, the S@SG-CNT composite with a mass loading of 2.6 mg cm-1 displayed an initial capacity of 743.1 mAh g-1 and maintained
Comparison of the electrochemical property of the S@SG-CNT cathode and other S-based materials previously reported in the related literature in Li-S batteries
|Materials||S loading (mg cm-2)||Current density||Cycle number||After cycles specific capacity (mAh g-1)||Ref.|
|S@SG-CNT||2.6||0.2 A g-1||500||773||This work|
|Sulfur cathode||1.2||0.5 C||250||905|||
|SPAN||1.5||0.1 A g-1||100||~500|||
|S/CP@NCNT@CoS3||3||1.3 A g-1||400||680|||
To investigate the mechanism of the stable cycling performance of the S@SG-CNT composites, EIS measurements were carried out. Figure 5A exhibits the Nyquist plots before and after various cycling at
Figure 5. (A) Nyquist plot of the S@SG-CNT before and after cycling with the inset showing the equivalent circuit used for data fitting; (B) the cyclic voltammetry of S@SG-CNT at various scan rates; (C) b-values plotted of the S@SG-CNT for Peaks 1-3; (D) b-values plotted of the three composites; (E) linear fits of the peak current of the S@SG-CNT for three peaks; and (F) Li+ ion diffusion coefficient for three samples.
Sweep voltammetry analysis was carried out to further understand the superior electrochemical kinetics of the S@SG-CNT in Li-S cells. Figure 2F and Supplementary Figure 20A and Figure 2F and B and Figure 5B display the CV curves of the S@CNT, S@O-CNT, and S@SG-CNT electrodes at various scan rates (0.2-1.0 mV s-1), respectively. With the increasing of the scan rate, the S@SG-CNT cathode shows the least variation of Peaks 1-3 followed by S@CNT and S@O-CNT, demonstrating that the polarization of S@SG-CNT is smaller than those of S@CNT and S@O-CNT. The relationship between the peak current (i) and scan rate (v) is i = avb. In Figure 5C and D, the b-values of the S@SG-CNT are 0.61, 0.52, and 0.67 at Peaks 1-3, respectively, which are higher than those of S@CNT and S@O-CNT [Figure 2F and Supplementary Figure 20C and Figure 2F and D]. In addition, the diffusion Li+ ion rate (DLi+) can be qualitatively measured according the Randles-Sevcik equation (Ip = 2.69 × 105 n3/2 A DLi+1/2 v1/2 CLi+) based on the above sweep voltammetry analysis, where Ip is the strongest peak current, A is the area of electrolyte (1.13 cm2), v is the scan rate, CLi+ is the concentration of Li+, n is the transferring electron numbers, and DLi+ is the diffusion coefficient. The value of DLi+ is determined from the slope of the linear relations between Ip and v1/2 [Figure 5E and Figure 2F and Supplementary Figure 20E]. After calculation, the slope values of S@SG-CNT were 0.821, 1.447, and 2.017 and the corresponding DLi+ were 2.861 × 10-7, 7.978 × 10-7, and 1.388 × 10-6 cm2 s-1 for the three peaks, respectively, which are all larger than those of S@CNT and S@O-CNT, suggesting the fastest intercalation/de-intercalation of Li+ in S@SG-CNT (see Figure 5F).
Furthermore, the four-point probe method was employed to investigate the influence of the unique 1D CNT/2D-stripped-G structure on the electrical conductivity of the CNT, O-CNT, and SG-CNT matrices. As shown in Figure 6A, the electronic conductivity of SG-CNT (7.9 S cm-1) was the highest, followed by GCNT (3.3 S cm-1) and O-CNT (2.5 S cm-1). This result strongly supports that the 3D cross-linked structure in the S@SG-CNT can enable fast electron/ion transfer through the 3D robust building blocks.
Figure 6. (A) Electrical conductivity of three matrices; (B) TEM image and (C) EDS spectrum of S@SG-CNT after 2000 cycles; (D) visualized adsorption of Li2S6 solution; and (E) schematic illustration of the electrochemical reaction mechanism of S@SG-CNT.
To analyze the structural properties of the S@SG-CNT after undergoing 2000 cycles, TEM was also employed. As shown in Figure 6B, the S@SG-CNT composite still maintained its initial 1D tube@2D sheets interconnected morphological structure at the current density of 2.0 A g-1 after 2000 cycles, indicating its morphology was not damaged during the electrochemical cycles. In addition, the S content [Figure 6C] was not obviously changed after long time cycling, further suggesting that the strong chemical interaction between S and SG-CNT matrix could immobilize S and alleviate the shuttle effect during the discharge/charge process in Li-S batteries and further contribute to a high stable cycling battery performance. To further explore the influence of the different matrices on the trapping capability of LPS, the Li2S6 adsorption test was performed. As shown in Figure 6D, the solution with SG-CNT was entirely decolored after 0.5 h, while the solutions with CNT and O-CNT showed less discoloration, demonstrating that SG-CNT with abundant OFG, especially the hydroxyl functional groups, exhibited an excellent binding capability of LPS compared to CNT and O-CNT. Based on the above analysis, the S@SG-CNT frameworks with 3D cross-linked, hierarchical pore structure not only serve as electron channels for fast electrochemical response but also enhance the interaction between S and matrix, thereby leading to superior electrochemical kinetics compared to those of S@CNT and S@O-CNT, as illustrated in Figure 6E and
In summary, a 3D SG-CNT matrix with hierarchical pore and abundant oxidative functional group structure was successfully prepared via an oxidation-assembly-reduction method. The unique 3D SG-CNT matrix was used as a smart building block to load S through a high-temperature infiltration technique to form S@SG-CNT cathode composites for Li-S battery. The S@SG-CNT cathodes with high S loading presented high reversible specific capacity and excellent rate cycling stability. The exceptional electrochemical performances of S@SG-CNT electrodes in Li-S battery is because: (1) the 1D/2D interwoven structure (1D CNT and 2D stripped-G) can provide excellent electrical conductivity, ensuring the rapid electrochemical response and shorten Li+ diffusion distance; (2) the hierarchical pores are not only suitable for high S loading but also effectively control the shuttle effect and buffer the volume change of S and structural expansion/shrinkage during long cycling process; and (3) the existence of oxidative functional groups, especially the hydroxyl groups, and the robust S-O chemical bonds on the carbon matrix surface can effectivity alleviate the diffusion of LPS into the organic electrolyte during the redox reactions. It is believed that the facile introduction of the hierarchical pore to carbonaceous host materials can pave a promising avenue for a high-performance Li-S battery.
Conceptualization, formal analysis, investigation, writing - original draft, review, and editing: Ruan J
Investigation, writing - original draft: Sun H
Formal analysis, writing - review and editing: Song Y
Formal analysis, investigation, writing - review and editing: Pang Y
Resources, writing - review and editing: Yang J
Supervision, resources, writing - review and editing: Sun D
Supervision, investigation, resources, writing - review and editing: Zheng SAvailability of data and materials
Not applicable.Financial support and sponsorship
We gratefully acknowledge the support of the National Natural Science Foundation of China (51971146, 51971147 and 52171218), the Shanghai Municipal Science and Technology Commission (21010503100), the Innovation Program of Shanghai Municipal Education Commission (2019-01-07-00-07-E00015), the General Program of Natural Science Foundation of Shanghai (20ZR1438400), and the Shanghai Rising-Star Program (20QA1407100), and the Postdoctoral Innovation Talents Support Program of China (BX2021067). We also acknowledge the support of Shanghai Outstanding Academic Leaders Plan and the Guangxi Key Laboratory of Information Materials (Guilin University of Electronic Technology, 201017-K).Conflicts of interest
All authors declared that there are no conflicts of interest.Ethical approval and consent to participate
Not applicable.Consent for publication
© The Author(s) 2021.
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