Fuhui
Wang
ab,
Weiyue
Jin
ab,
Zecheng
Xiong
ab and
Huibiao
Liu
*ab
aBeijing National Laboratory for Molecular Sciences, CAS Research/Education Center for Excellence in Molecular Sciences, CAS Key Laboratory of Organic Solids, Institute of Chemistry, Chinese Academy of Sciences, Beijing 100190, P. R. China. E-mail: liuhb@iccas.as.cn
bUniversity of Chinese Academy of Sciences, Beijing 100049, P. R. China
First published on 18th May 2021
Manganese dioxide (MnO2) has been demonstrated to be a promising cathode material for aqueous zinc-ion batteries (ZIBs) due to its low cost, good safety and high output voltage; however, it suffers from an intrinsically low electrical conductivity, poor rate performance and rapid capacity deterioration. Herein, a new kind of MnO2@GDYO hybrid three-dimensional (3D) nanoflower has been designed and fabricated via the in situ growth of MnO2 in graphdiyne oxide (GDYO) nanosheets in aqueous solution. The MnO2@GDYO hybrid 3D nanoflowers have the dual advantages of MnO2 and GDYO, which effectively improve the electrochemical activity and reversibility, increase the ion-/electron-transport channels and enhance the structural stability. Meanwhile, the unique 3D nanoflower structure has large specific surface area, shortens the ion-transport distance and improves the electrochemical reaction kinetics. The rechargeable aqueous Zn//MnO2@50GDYO battery presents an admirable capacity of 253.7 mA h g−1 at 1C, a superior rate capacity of 80.6 mA h g−1 at 10C, and excellent operating stability over 1000 cycles at 5C with a capacity retention of 77.6% and a coulombic efficiency approaching 100%. The facile preparation and excellent electrochemical performance make hybrid-based graphdiyne oxide a promising candidate as a cathode for high-performance ZIBs.
There are some strategies for improving the performance of ZIBs based on MnO2, such as the pre-addition of Mn2+ salt in mild aqueous electrolytes for suppressing the dissolution of Mn2+ and improving the cycling stability of MnO2 cathodes,11,12 developing MnO2 materials with a vast variety of polymorphs (i.e., α-, β-, γ-, and δ-MnO2),13,14 and investigating different morphologies (i.e., nanowires,15 nanorods,16 nanospheres17 and nanoflakes18) and their hybrids (i.e., MnO2/graphene,19 MnO2/graphite,20 MnO2/carbon nanotube21 and MnO2/polyaniline22), which have resulted in preliminary achievements. The nanostructural MnO2 can provide an enlarged electrolyte/electrode contact area, increase the number active sites and shorten ion-/electron-diffusion pathways for promotion of the capacity and reaction kinetics of MnO2. Various nanostructures of MnO2 exhibit good electrochemical performances in either batteries or supercapacitors.23–25 Hybridizing MnO2 with carbon materials has been considered as an effective approach to improve its electronic conductivity, structural stability and to accommodate the structural change during the cycling process. Various carbon materials, including graphene, carbon nanotubes and graphite, exhibit superb electrical conductivity when applied in aqueous ZIBs. However, most of the MnO2/conductive additive composites prepared by physical mixing methods such as ultrasonic mixing,26 ball milling,27 and vacuum filtration28,29 have an obvious phase-separation interface after repeated discharge–charge cycles, which brings about the loss of good conductive contact and internal structure stability. Therefore, it is imperative to introduce new carbon materials and develop new efficient and reliable methods for the preparation of homogeneous hybrid materials based on MnO2 and novel carbon materials.
Graphdiyne (GDY) is a novel 2D carbon allotrope with benzene rings connected by butadiyne linkages (–CC–C
C–) to form 18-C hexagons and has displayed excellent electrical, catalytic and optical properties.30–32 The extended existence of sp- and sp2-hybridized carbon atoms endows GDY with a 2D planar structure, uniformly distributed pores, excellent electrical conductivity, high chemical stability and so on.33–35 Graphdiyne oxide (GDYO) is one of the important derivatives of GDY, and is prepared by surface oxidation with an oxidizing agent. GDYO preserves the integrity of the skeletal 2D structure of GDY (C
C, C
C) to ensure a rich pore structure with uniform distribution, and forms abundant hydrophilic oxygen-containing functional groups (C
O) on its basal planes and edges, which are beneficial to guest metal ions, chelating them firmly. Herein, we develop an in situ growth strategy to construct MnO2@GDYO hybrid 3D nanoflowers using GDYO nanosheets. With abundant nanopores in each GDYO skeleton plus the porous network composed of the interconnected GDYO nanosheets, the integrated MnO2@GDYO hybrid 3D nanoflowers provide numerous channels for the transport of ions/electrons, enhanced charge-transfer kinetics and structural stability. In addition, the 3D nanoflower is capable of greatly enlarging the electrolyte/electrode contact area, increasing the number of active sites and shortening the ion-/electron-diffusion pathways. Furthermore, the size, surface area and morphologies of MnO2@GDYO hybrid 3D nanoflowers can be tuned by controlling the conditions of in situ growth, which results in the controllable performance of aqueous ZIBs. The as-prepared MnO2@50GDYO hybrid 3D nanoflowers used as a cathode for aqueous ZIBs exhibit a superior rate capability of 80.6 mA h g−1 at 10C and an excellent cycling stability of up to 1000 cycles with a capacity retention of 77.6%, a coulombic efficiency approaching 100% and a high capacity of 253.7 mA h g−1 at 1C. This work brings new prospects for the design of GDYO hybrids for high-performance rechargeable aqueous ZIBs.
The morphology and structure of the MnO2@GDYO hybrid 3D nanoflowers were characterized by SEM and TEM (Fig. 2 and Fig. S2–S4, ESI†). From the SEM images, the evolution of the MnO2@GDYO nanostructures indicates that the morphologies are well controlled. With an increase in the amount of GDYO, the formation of thinner and finer 3D nanoflower structures of MnO2@GDYO hybrids are promoted compared with bare MnO2 (Fig. S5, ESI†). Fig. 2 shows the typical morphology of MnO2@50GDYO, which is composed of agglomerated nanoflowers with ample wrinkles and folds. There was no obvious exposure of GDYO nanosheets, which confirmed that all MnO2 grew on the surface of GDYO, covering it completely, and there was no separated phase interface as illustrated in Fig. S6 (ESI†). Such an interconnected network not only ensures the electrochemical activity but also enhances the integral mechanical stability. More detailed structural information can be obtained by TEM, and all of the MnO2@GDYO hybrids display a thin sheet-like morphology which folds up into complex 3D nanoflower structures. When the content of GDYO is too low, the morphology of the MnO2@10GDYO hybrid is close to that of MnO2, which has a thicker and larger sheet aggregated structure. With the increase of GDYO content, the degree of cross-linking between MnO2 and GDYO increases, gradually forming the ultra-thin sheet aggregate structure. However, when the amount of GDYO is too high, the MnO2@100GDYO hybrid aggregates severely, covering the exposed surface of the ultrafine structure, and resulting in a decrease in the specific surface area and pore structure. The TEM images of the MnO2@50GDYO hybrid indicate that the flower-like structures are constructed from nanosheets, consistent with the SEM observations. High-resolution TEM (HR-TEM) characterization of the MnO2@50GDYO hybrid is shown in Fig. 2f, and the lattice spacings of 0.24 nm and 0.48 nm are found to match well with the (006) and (004) crystal planes, respectively, of birnessite-MnO2. Moreover, energy dispersive X-ray spectroscopy (EDS) mapping images (Fig. 2g) with respect to Mn, O and C show that these elements are abundant and well-distributed throughout the nanoflower, suggesting that the MnO2 grows uniformly on the GDYO surface. Similar results were obtained in the MnO2@10GDYO, MnO2@20GDYO, and MnO2@100GDYO hybrids.
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Fig. 2 Microstructural and compositional analysis of the MnO2@50GDYO hybrid 3D nanoflowers: (a–c) SEM images; (d and e) TEM images; (f) HR-TEM image; and (g) elemental mapping images of Mn, O and C. |
The crystallographic structures of the MnO2@GDYO hybrid 3D nanoflowers were confirmed by XRD. As shown in Fig. 3a and Fig. S7 (ESI†), all of the diffraction peaks can be well indexed to pure phase birnessite-MnO2 (JCPDS 18-0802) and GDYO. The peaks at 12.1°, 24.7°, 36.5°, 53.2° and 65.6° are related to the (002), (004), (006), (301) and (119) planes of birnessite-MnO2, respectively. GDYO exhibits a broad diffraction peak around 23°, which is ascribed to the typical interlayer distance of the GDY material.37,38 In addition, the XRD patterns for the MnO2@GDYO hybrid 3D nanoflowers present less noticeable peaks for MnO2 and a high peak for GDYO, showing the combination of MnO2 and GDYO. It is noticeable that the peaks with a broad feature and low intensity are indicative of the nanoscale structure and low crystallinity of the MnO2@GDYO hybrid 3D nanoflowers, which is in line with the HR-TEM observations. In particular, when the GDYO content reached 100 mg, the corresponding (002) and (004) diffraction peaks in the XRD pattern almost disappeared, and the lattice spacing of 0.48 nm was not observed in the HR-TEM image (Fig. S4f, ESI†).
To further characterize the composites, Raman analysis was carried out. As shown in Fig. 3b and Fig. S8 (ESI†), a sharp peak is seen at 648 cm−1, which can be attributed to the symmetric Mn–O stretching vibrations of the MnO6 octahedron in MnO2, similar to those previously reported.39 In addition, in the spectrum of the MnO2@GDYO hybrid 3D nanoflowers, the prominent peaks of GDYO are seen at 1378 and 1589 cm−1, corresponding to the defect-induced (D band) and graphitic-induced (G band) carbon structures, respectively, demonstrating the presence of MnO2 and GDYO.
XPS measurement was carried out to investigate the chemical composition and the electronic states of the MnO2 and MnO2@GDYO hybrid 3D nanoflowers. The existence of elemental C, O, and Mn signals are obvious from the full-scan XPS spectrum (Fig. 3c), suggesting the presence of manganese oxide and carbon materials. The C 1s peak of the MnO2@50GDYO hybrid 3D nanoflowers can be deconvoluted into four subpeaks of CC (sp2), C
C (sp), C–O, and C
O at 284.4, 285.0, 286.2, and 288.8 eV, respectively (Fig. 3d), consistent with the expected chemical composition of GDYO.40 The deconvoluted O 1s spectrum shows that five components appear at 529.65, 530.77, 531.8, 532.51 and 533.5 eV (Fig. 3e), which are in turn indexed to Mn–O–Mn bonds for the tetravalent oxide, Mn–O–H bonds for a hydrated trivalent oxide, C
O bonds for the carboxyl groups on the surface of GDYO, H–O–H bonds for residual water and –OH bonds for the hydroxyl groups on the surface of GDYO, respectively. The peak splitting of the doublet in the Mn 3s core-level spectrum is about 5.04 eV, suggesting that Mn4+ is dominant in the MnO2@50GDYO hybrid 3D nanoflowers. Moreover, the shoulder peaks of Mn 2p in Fig. 3g are characteristic of Mn 2p1/2 (653.9 eV) and Mn 2p3/2 (642.2 eV), agreeing well with the typical spin energy separation of 11.7 eV for MnO2.41 The same results for MnO2@10GDYO, MnO2@20GDYO and MnO2@100GDYO have been obtained and are presented in Fig. S9 (ESI†). The results clearly confirm that the MnO2@GDYO hybrid 3D nanoflowers were successfully prepared.
TGA was used to study the content of GDYO in the MnO2@GDYO hybrid 3D nanoflowers (Fig. 3h and Fig. S10, ESI†). The weight loss below 240 °C is derived from the removal of adsorbed water, and the subsequent decrease originates from the combustion of GDYO to CO2.16 For MnO2, a weight loss of about 5% is observed in the range of 240–500 °C, which is attributed to the phase transformation of MnO2.42 By calculation, we estimated that the mass percentage of GDYO in the MnO2@50GDYO hybrid 3D nanoflowers is about 10.53%. The results for the GDYO mass percentage obtained in the MnO2@10GDYO, MnO2@20GDYO and MnO2@100GDYO hybrid 3D nanoflowers are about 3.79%, 5.91%, 16.92%, respectively.
Fig. 3i shows the nitrogen adsorption–desorption isotherm of the MnO2@50GDYO hybrid 3D nanoflowers, in which the remarkable hysteresis loop in the intermediate P/P0 range illustrates a unique mesoporous texture and the BET specific surface area is as high as 204.83 m2 g−1, exceeding that of the pure MnO2 (77.93 m2 g−1). The measured value is higher than those reported for MnO2 prepared using other synthetic routes (Table S1, ESI†). The samples with different GDYO contents all showed similar hysteresis loops with mesoporous dominant structural characteristics, and the BET specific surface areas are calculated as 81.85 (MnO2@10GDYO), 130.53 (MnO2@20GDYO), and 128.30 m2 g−1 (MnO2@100GDYO) (Fig. S11 and S12, ESI†). In particular, the use of excessive GDYO resulted in agglomeration, a smaller specific surface area and a larger volume expansion for MnO2@100GDYO (Fig. S13, ESI†). It is believed that the mesoporous architecture and the large specific surface area of MnO2 can not only promote the swift diffusion, transportation, and intercalation of electrolyte ions throughout the electrode, but also accommodate the volume change of MnO2 during the charging–discharging processes.43
To investigate the electrochemical performance of the MnO2@GDYO hybrid 3D nanoflowers as a cathode for aqueous ZIBs, coin-type cells were assembled using Zn foil as the anode. Fig. 4a exhibits the CV curves of MnO2 and MnO2@GDYO electrodes at a scan rate of 0.1 mV s−1. There are two couples of redox reactions, indicating that the ZIBs undergo a two-step electrochemical process. It should be noted that GDYO makes no capacity contribution to zinc ion storage as shown in Fig. S14a and b (ESI†). Fig. 4b presents the rate performances tested at different current densities, and corresponding cycle profiles are given in Fig. 4d and Fig. S14c–f (ESI†). In addition to MnO2@100GDYO, MnO2 and other MnO2@GDYO electrodes have an approximate specific capacity at 0.1C, indicating that the excess GDYO actually reduces the specific capacity of the battery. Although MnO2@100GDYO cathode makes a higher capacity retention rate, it comes at the cost of specific capacity. In the process of developing electrode materials, the specific capacity should be considered as well as the rate performance. When the GDYO amount is increased to 50 mg, both the specific capacity and the rate capability stand out among the five samples. Therefore, the optimized hybrid MnO2@50GDYO is used for the following study. As shown in Fig. 4b, the MnO2@50GDYO cathode delivers the capacities of 265.1, 272.3, 273.8, 243.0, 204.3, 127.4, and 80.6 mA h g−1 at discharge–charge rates of 0.1, 0.2, 0.5, 1, 2, 5 and 10C (based on the active mass of MnO2), respectively. More importantly, when the current rate switches back to 1C, the capacity recovers to 253.7 mA h g−1, which is 95.7% of the value at 0.1C. The high-rate capability is not only superior to the corresponding values for the control electrodes as displayed in Fig. 4c, but is also comparable to those of known MnO2 cathode materials reported previously (Table S2, ESI†). This outstanding rate performance can be understood based on the EIS results of MnO2 and MnO2@GDYO electrodes, and the resulting Nyquist plots were fitted by the inset equivalent circuit (Fig. S15a, ESI†). The high frequency semi-circle corresponds to the charge-transfer resistance (Rct), the low-frequency inclined line stands for the Warburg impedance (Zw) and R0 is the series resistance of the electrochemical system. The detailed EIS information is shown in Table S3 (ESI†). According to the results, the MnO2@GDYO electrodes exhibit significantly smaller R0 and Rct values, and a lower Warburg diffusion resistance (the steeper slope). As a consequence, the introduction of the GDYO in the in situ grown MnO2 can effectively enhance the charge-transfer ability, and thereby accelerate the electrode reaction kinetics for a high rate performance. The excellent rate performance also can be attributed to the 3D flower-like MnO2@GDYO nanostructures, which provide a high specific surface area for more active sites and a unique mesoporous nanotexture for ion-diffusion channels as well as the porous nature of GDYO. The specific capacity could return to the initial level when the current density is switched back to a current rate of 1C, again confirming the high reactivity and reversibility of the MnO2@GDYO cathodes. In addition to the excellent rate capability, the MnO2@GDYO cathodes also possesses remarkable cyclability. Fig. 4e compares the cycling performance of MnO2 and MnO2@GDYO cathodes at 1C. Dramatic capacity fading can be clearly observed from the cycling curves of MnO2 in the initial cycles. The MnO2@GDYO cathodes all have an excellent cycle stability, but the presence of excessive GDYO will reduce its specific capacity, for example, the specific capacity of MnO2@100GDYO hybrid is only 215 mA h g−1 at 1C. The higher specific capacity of the MnO2@GDYO cathodes is due to the larger specific surface area and higher number of active sites of the MnO2@GDYO hybrid 3D nanoflower material. Serious aggregation of MnO2@100GDYO hybrid leads to a decrease in specific surface area, which in turn leads to a decrease in the specific capacity. The structural stability of the MnO2@GDYO cathodes was strengthened by the ingenious in situ induction growth strategy, and the cycling and rate properties of the MnO2@GDYO cathodes were significantly improved. Of the five electrodes, the MnO2@50GDYO hybrid clearly exhibits the best cycling performance (239 mA h g−1 after 50 cycles, a capacity retention ratio of 99.2% at 1C), even after cycling for over 150 cycles (Fig. S16, ESI†). The long-term cycling stability with quite a high current density of 5C over 1000 cycles shows a remarkable capacity retention of 77.6% and coulombic efficiency approaching 100% (Fig. 4f). After the discharge–charge testing, postmortem analysis shows that the electrode retains the nanoflower morphology, indicating the strong structural stability of the MnO2@GDYO hybrids (Fig. S17, ESI†).
The fundamental energy-storage mechanism of the MnO2@GDYO cathodes, using MnO2@50GDYO as an example, during electrochemical cycling is investigated by ex situ XRD, SEM and XPS measurements to unveil the phase and microstructural evolution. Fig. 5a shows the typical charge–discharge curves for the initial two cycles marked with different states from A to I. During the initial discharging (A–B–C), the corresponding XRD patterns exhibit diffraction peaks at 19° and 35°, which belong to MnOOH (JPCDS 18-0804) (Fig. 5b and Fig. S18, ESI†), formed because of the reaction of proton insertion into manganese dioxide, H+ + MnO2 + e− → MnOOH. The gradual depletion of H+ would lead to an enrichment of OH− surrounding the cathode and thus the subsequent OH− react with ZnSO4 and H2O in the aqueous electrolyte, 6OH− + 4Zn2+ + SO42− + 3H2O → Zn4SO4(OH)6·3H2O.44–46 From this, a new phase with characteristic 2θ peaks at around 10°, 21°, 22°, 26°, 28°, and 59° appear in the discharge plateau, which can be assigned to zinc sulfate hydroxide hydrate (Zn4SO4(OH)6·3H2O, JPCDS 39-0689). With deep discharging to 1.0 V (C and G), the peak intensity of Zn4SO4(OH)6·3H2O increases, indicating the growth of the Zn4SO4(OH)6·3H2O structure. As displayed in Fig. 5c and Fig. S18 (ESI†), the ultrathin nanosheets evolve into large size micro-sheets and a white substance can be observed on the electrode surface. Compared with the original state, a new diffraction peak emerges at 33°, which depicts the formation of ZnMn2O4 (JCPDS 24-1133). This can be attributed to the insertion of Zn2+ into the MnO2 tunnels, accompanied by the valence decrease of positive quadrivalent manganese (Fig. 5d and Fig. S19, ESI†), Zn2+ + 2MnO2 + 2e− → ZnMn2O4. HR-TEM EDS mapping of the MnO2@50GDYO cathode in a fully discharged state offers further proof of the insertion of Zn2+, while the Zn signal is seen uniformly everywhere (Fig. 5e). In the reverse charging process (C–D–E, G–H–I), the extraction of H+ and Zn2+ from the electrode could result in the dissolution of the Zn4SO4(OH)6·3H2O phase. Both the diffraction peaks of the Zn4SO4(OH)6·3H2O phase and the micro-sheets disappear, revealing a reversible precipitation–dissolution of the Zn4SO4(OH)6·3H2O structure. A reversible precipitation–dissolution process can be maintained even after long-term cycle testing, as shown in Fig. S20 (ESI†). Therefore, the energy-storage mechanism is a co-insertion/extraction process of Zn2+ and H+ into MnO2 accompanied by the precipitation–dissolution of the Zn4SO4(OH)6·3H2O phase.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d1qm00548k |
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