Jianbiao Wang†
*a,
Peidian Chong†b,
Wanwisa Limphirat†c,
Haiyi Wanga,
Wutthikrai Busayaporn
c,
Lei Zhang
a,
Debbie Hwee Leng Senga,
Shengnan Sun
a,
Zainul Aabdin
a,
Chaoyu Dongd,
Mingdeng Wei
*b and
Zhi Wei Seh
*a
aInstitute of Materials Research and Engineering (IMRE), Agency for Science, Technology and Research (A*STAR), 2 Fusionopolis Way, Innovis #08-03, Singapore 138634, Republic of Singapore. E-mail: jianbiao_wang@imre.a-star.edu.sg; sehzw@imre.a-star.edu.sg
bFujian Key Laboratory of Electrochemical Energy Storage Materials, Fuzhou University, Fuzhou 350116, China. E-mail: wei-mingdeng@fzu.edu.cn
cSynchrotron Light Research Institute, 111 Moo 6 University Avenue, Muang, Nakhon Ratchasima 30000, Thailand
dSingapore Institute of Manufacturing Technology (SIMTech), Agency for Science, Technology and Research (A*STAR), 5 Cleantech Loop, 01-01 Cleantech Two Block B, Singapore 636732, Republic of Singapore
First published on 31st July 2025
Sodium-ion batteries (SIBs) have been intensively researched as potential alternative energy storage devices to lithium-ion batteries (LIBs). Nevertheless, the scarcity of suitable anode materials capable of hosting the large radius of Na+ has hindered the further application of SIBs. Herein, we developed a hierarchical VS4 nanosheet with an expanded interchain spacing of 0.98 nm without additives for the first time. Additionally, we found that the porous structure in the hierarchical VS4 nanosheet provides sufficient active sites for Na+ storage and alleviates the volume variation during discharge/charge cycles, as supported by finite element simulation (FES) data. More importantly, a dynamic insertion-dominated storage mechanism was revealed through synchrotron X-ray absorption spectroscopy and X-ray photoelectron spectroscopy. Thus, the optimized anode delivered a high capacity of 441 mAh g−1 at 1 A g−1 after 200 cycles. This work provides critical insights into the design of SIBs by correlating storage mechanisms with electrode's structural composition.
The electrochemical kinetics of SIBs can be enhanced by employing transition metal sulfides as anodes, owing to their high theoretical capacity and excellent ionic conductivity.7,18–20 Among these, VS4 has emerged as a promising candidate, as its abundant (S2)2− anions contribute to high capacity. However, its practical application is hindered by significant volume changes during the discharge/charge process.21–24 To address this challenge, various strategies have been explored, such as combining VS4 with MXenes or fabricating heterojunction structures.25 However, achieving high capacity VS4-based anodes remains challenging.
Ether-based electrolytes with sodium trifluoromethanesulfonate (NaOTF) have been extensively researched in SIBs due to high reversibility during plating/stripping of Na+.6,9 A limited understanding of the storage mechanisms of VS4 in NaOTF-ether electrolytes also further constrains its application in SIBs.
Here, for the first time, we synthesized hierarchical VS4 nanosheets with expanded interchain spacings via a one-step solvothermal process, without the need for any additives. To the best of our knowledge, this work reports the largest interchain spacing for VS4 to date, offering increased Na+ storage capacity. Unlike previous studies, we unveiled a dynamic insertion-dominated storage mechanism in the discharge/charge process with NaOTF-ether electrolyte, using synchrotron X-ray absorption spectroscopy (XAS) and X-ray photoelectron spectroscopy (XPS). Additionally, the porous structure provides ample space to accommodate Na+ and mitigates the volume variation in the insertion/extraction of Na+, enhancing structural stability, as supported by finite element simulation (FES) data. The presence of nanosheets can effectively reduce the diffusion pathway of Na+. Moreover, the composition of the solid electrolyte interface (SEI) formed on the surface of VS4 nanosheets was also investigated using XPS. Thus, a stable electrochemical performance of VS4 could be achieved. In detail, the hierarchical VS4 nanosheet anode retains a high capacity of 441 mAh g−1 at 1000 mA g−1 after 200 cycles, showing advantages among VS4-based anodes.19 Based on this work, we found that the interfacial chemistry between the electrode and electrolyte is vital for the cycling performance of batteries. Future efforts will focus on investigating and optimizing SEI formation to advance the development of high-energy-density batteries.
As presented in Fig. 2a, most reflections in the XRD pattern are well indexed to standard reference of VS4. Notably, the characteristic peak of the (110) plane is observed to be shifted to 8.8°, and the corresponding interchain spacing is calculated to be 0.99 nm based on the Braggs law equation.16 The calculated expanded interchain spacing is greater than previous reported spacing, agreeing well with TEM observation.19,20 This is also the first report of such a large interchain spacing in VS4, which could allow for more Na+ to insert into the structures. The observed bands at 139 cm−1, 191 cm−1, 281 cm−1, and 405 cm−1 from the Raman spectrum are ascribed to characteristics of VS4 (Fig. 2b).26,27 The survey X-ray photoelectron spectra confirmed the presence of V and S elements in VS4 (Fig. S1). The curve-fitted peak components of V 2p at 524.2 eV and 516.8 eV, as well as 521.2 eV and 513.7 eV, are associated with V4+ and V3+, respectively, which agrees well with previous reports.28–30 Curve fitting of the S 2p spectrum yields three peaks: the binding energies at 163.5 eV and 162.3 eV are assigned to S 2p1/2 and S 2p3/2 of (S2)2−, respectively, while the binding energy at 161.1 eV is related to S2−.21,22,27 These characterization results confirmed the successful preparation of hierarchical VS4 nanosheets.
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Fig. 2 Materials characterization: (a) XRD pattern, (b) Raman spectrum, and XPS spectra of (c) V 2p and (d) S 2p, respectively. |
To gain deeper insight into the formation mechanism of hierarchical VS4 nanosheets, we have conducted experiments with different reaction times of 10 min, 30 min, and 1 h. Then we collected the TEM images and corresponding maps of these samples, as demonstrated in Fig. S2–4. Based on these observations, we propose the formation mechanism of hierarchical VS4 nanosheets, as demonstrated in Fig S5. The evolution of crystallinity is revealed by XRD patterns with different reaction times (Fig. S6). The characteristic reflections of VS4 appeared when the reaction time reached up to 2 h.
We conducted a series of electrochemical tests to evaluate the effectiveness of the designed hierarchical VS4 nanosheets in hosting Na+. CV curves were obtained at 0.5 mV s−1, in which the decreased voltage gap of redox peaks could be observed upon cycling (Fig. 3a). Moreover, the increasing intensity of redox peaks in the CV curves over successive cycles indicates reduced polarization and accelerated kinetics. Thereafter, the cycling performance was tested at 500 mA g−1, and a stable capacity of 509 mAh g−1 is achieved after 110 cycles (Fig. 3b). Even at a higher current density of 1000 mA g−1 (Fig. 3c), the electrode can retain a high capacity of 441 mAh g−1 after 200 cycles, showing some advantages among reported VS4-based anodes in SIBs (Table S1).21,31–41 Furthermore, the plateaus observed in corresponding charge–discharge profiles at 1000 mA g−1 agree well with the redox peaks in CV curves. Moreover, the charge–discharge profiles after the 100th cycle demonstrate the smallest voltage gap between discharge and charge plateaus compared to the 10th and 50th cycles, further supporting the enhanced kinetics as observed in CV curves (Fig. 3d). In contrast, the electrode is short-circuited after 43 cycles with an inferior capacity of 75 mAh g−1 when it was used in electrolytes based on NaPF6, reflecting the advantages of NaOTF electrolytes (Fig. S7). CV measurements at varying scan rates were performed to investigate the capacity contribution dominated by the diffusion-controlled process or the capacitance effect, based on the following equation:
i = avb | (1) |
i = k1v + k2v1/2 | (2) |
XPS depth profiling and synchrotron XAS spectra are used to understand the storage mechanism and interfacial chemistry between hierarchical VS4 nanosheets and electrolytes (Fig. 4–7). Ex situ XPS spectra were collected from samples at different potential states of 1.5 V, 0.01 V, 2.0 V, and 3.0 V. The data labelled 1.5 V, 1.5 V–3, and 1.5 V–5 represent samples treated with etching times of 0 min, 3 min, and 5 min, respectively (the notation applies to other potential states as well). Upon discharge to 1.5 V, the intensity peaks for V4+ increase, while those for V3+ decrease, in contrast with the pristine sample. This should be attributed to insertion of Na+ and transfer of electrons within VS4 and formation of Na3VS4.21 No significant differences in V 2p are observed among the 1.5 V, 1.5 V–3, 1.5 V–5 samples. Upon further discharge to 0.1 V, the intensity ratio for V4+/V3+ increases at the electrode surface, while it decreases in both 0.1 V–3 and 0.1 V–5. This suggests the co-existence of insertion/conversion reactions during the discharge process, with the high V4+/V3+ intensity ratio at 0.1 V likely attributed to the surface oxidation in the process of measurements.
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Fig. 4 Ex situ XPS spectra of V 2p from samples at different potential states of (a) 1.5 V, (b) 0.1 V, (c) 2.0 V, and (d) 3.0 V. |
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Fig. 5 Ex situ XPS spectra of S 2p collected at different voltages of (a) 1.5 V, (b) 0.1 V, (c) 2.0 V, and (d) 3.0 V, respectively. |
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Fig. 6 Ex situ XPS spectra of F 1s collected at different voltages of (a) 1.5 V, (b) 0.1 V, (c) 2.0 V, and (d) 3.0 V, respectively. |
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Fig. 7 (a) XAS spectra collected at different potential states, and (b) corresponding magnified part of the K-edge. |
During the subsequent charge process, the binding energies of V 2p at 2.0 V are higher than those at 1.5 V and 0.1 V, which comes from the presence of V5+.28 More importantly, the binding energies of V 2p at 2.0 V–3 and 2.0 V–5 are similar but higher than those at 2.0 V, suggesting that the degree of insertion reaction is greater within the bulk of the material than at the surface. Upon full charging to 3.0 V, the V 2p binding energies shift further to higher values, demonstrating partial reversibility of the insertion reactions. These results suggest that Na3VS4 remains partially unconverted, with only partial reversibility of the conversion reactions. Therefore, the final product at the full charge state is likely a composite of Na3VS4 (V5+) and VS4 (V4+), which is different from previous reports that use NaOTF-based ether electrolyte.21,30
We have also investigated the composition of solid electrolyte interphase (SEI) formed on the surface of the anode after two cycles (Fig. 6 and S10). In detail, the deconvoluted F 1s spectra show binding energies at 688.5 eV and 683.7 eV, corresponding to Na–F and C–F bonds, respectively.11,42 The disappearance of the C–F peak after the etching treatment suggests that the C–F bonds originate from electrolytes. Moreover, the binding energy for Na–F binding can be observed at different etching times, indicating the formation of a stable NaF-rich SEI layer. The corresponding Na 1s XPS spectra collected from different potential states also supported the presence of a SEI formed on hierarchical VS4 nanosheets, accounting for the superior electrochemical sodium storage performance.
XAS spectra at different potential states were collected to gain a deeper understanding of the energy storage mechanism (Fig. 7a and b). The K-edge of V shifts to higher photon energy in contrast to the sample at open circuit voltage (OCV) throughout the discharge/charge process, which is attributed to the insertion of Na+ and the formation of Na3VS4. Notably, at a discharge cut-off voltage of 0.1 V, the V K-edge approaches that of OCV, suggesting a hybrid mechanism involving both conversion and insertion. In the converse charge potential states of 0.8 V and 3.0 V, the V K-edges further shift to higher energy regions relative to 0.1 V and OCV. These observations confirm that the insertion reactions dominate the entire electrochemical process at the bulk level, aligning well with ex situ XPS results.
To highlight the advantages of hierarchical VS4 nanosheets, we compared the stress and corresponding displacements between solid spheres and hierarchical nanosheet structures of VS4 under free boundary conditions (Fig. 8). The average stress in solid spheres and hierarchical nanosheets is simulated to be similar (Fig. 8a and c). However, the average displacement in solid spheres (22.8 nm) is higher than that in hierarchical nanosheets (19.8 nm) (Fig. 8b and d). Notably, displacement in the hierarchical nanosheets is mainly located at the outer edges, providing sufficient space to allow for volume change. In contrast, there is no space for solid spheres to undergo expansion, making them prone to cracking during cycling. So, these results demonstrate that the rational design of hierarchical nanosheets effectively mitigates mechanical stress and enhances electrochemical performance.
Computer tomography (CT) of pouch cells before cycling and after 20 cycles is used to investigate the volume changes of hierarchical VS4 nanosheets (Fig. S11). The cross-section CT slices show no significant change in the anode thickness after 20 cycles, which is consistent with the FES results. Moreover, the TEM image and corresponding elemental maps of the electrode after 20 cycles reveal that the hierarchical nanosheet morphology can be well retained, supporting the structural stability of hierarchical VS4 nanosheets (Fig. S12).
Supplementary information is available. See DOI: https://doi.org/10.1039/d5ta03608a.
Footnote |
† These authors contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2025 |