Open Access Article
Jinmin
Wang†
a,
Shuang
Wei†
bc,
Mingming
Fang
*b,
Angye
Li
d,
Qian
Zheng
a,
Xubing
Dong
b,
Yuanmao
Chen
b,
Kang
Yuan
b,
Xinyang
Yue
*b and
Zheng
Liang
*b
aSchool of Petrochemical Engineering, Changzhou University, Changzhou 213164, China
bFrontiers Science Center for Transformative Molecules, School of Chemistry and Chemical Engineering, Shanghai Jiao Tong University, Shanghai 200240, China. E-mail: 193679@sjtu.edu.cn; xinyangyue@sjtu.edu.cn; Liangzheng06@sjtu.edu.cn
cShanghai TANSUO Testing and Inspection Company, Shanghai 200240, China
dXi'an Jiaotong-Liverpool University, Suzhou 215000, China
First published on 6th January 2026
Sulfonyl-based compounds are considered promising electrolyte solvents because of their high dielectric constant, excellent anodic stability, and non-flammability. However, their use in Li metal batteries (LMBs) is limited by their incompatibility with Li, causing unstable interfacial chemistry and dendrite growth. Herein, we designed an N,N-dimethylsulfamoyl fluoride (DMSF) electrolyte by functionalizing a fluorosulfonyl (FSO2−) core with an N,N-dimethyl terminal group, enabling the LMB with enhanced cycling stability and energy density. The increased steric hindrance in DMSF with methylation weakens the interaction with Li ions, resulting in a structure that is weakly solvating and exhibits fast ion transport kinetics. Methylation also facilitates the decomposition of DMSF, leading to the formation of a rich LiF/Li2S hybrid solid electrolyte interphase that suppresses interfacial side reactions. Consequently, the 4.5 V-charged 50 µm Li‖LiNi0.8Co0.1Mn0.1O2 (4 mAh cm−2) cells exhibit stable cycling (80% capacity retention for 850 cycles), 5C fast charging, and a wide operating temperature range (−50–60 °C). Moreover, a 5-Ah pouch cell employing DMSF delivers an energy density of 540 Wh kg−1 and exhibits high stability over 110 cycles. This study establishes terminal group modification as a crucial advance for developing compatible sulfonyl-based electrolytes in high-performance LMBs.
Compared to the carbonyl group in carbonate solvents and the ether group in oligoethers, the strongly electron-withdrawing sulfonyl group significantly lowers the highest occupied molecular orbital (HOMO) energy level, thereby improving oxidation stability.25–28 However, using sulfonyl-based solvents in LMBs is still problematic because they have poor wettability and high viscosity and struggle to form a stable SEI on Li anodes.29–31 To enhance the compatibility, employing localized high-concentration electrolytes (LHCEs) or introducing functional groups into sulfonyl molecules has been demonstrated as an effective strategy with intriguing progress.32,33 Incorporating an N,N-dimethyl group into trifluoromethyl-containing sulfonyls can yield an electrolyte exhibiting good compatibility with both Li metal (coulombic efficiency > 99%) and high-voltage cathodes (>4.7 V vs. Li/Li+). Nevertheless, the combined steric hindrance from trifluoromethyl and N,N-dimethyl groups often reduces ionic conductivity at room temperature (1.5 mS cm−1), limiting ion transport and rate performance.34 Although Zhao and Kim et al. improved conductivity via mono-fluoro substitution, the electrochemical stability window was constrained to 4.3 V, which reduces the energy density of LMBs.35,36 In essence, innovative sulfonyl-based electrolytes that simultaneously achieve high energy density, superior rate performance, and wide temperature tolerance remain scarce yet are critically demanded for long-cycling, high-energy-density LMBs.
In this work, N,N-dimethylsulfamoyl fluoride (DMSF) characterized by the introduction of an N,N-dimethyl terminal group onto a fluorosulfonyl (FSO2−) core was proposed to improve compatibility between sulfonyl solvents and Li metal. The DMSF electrolyte was formulated by combining lithium bis(fluorosulfonyl)imide (LiFSI) and lithium hexafluorophosphate (LiPF6) at a molar ratio of LiFSI
:
LiPF6
:
DMSF = 1
:
0.1
:
5 (1.6 mol L−1). The synergistic integration of monofluoro and dimethyl functional groups imparts unique electronic and steric effects to the DMSF molecule. This configuration yields a weakly solvating structure that retains moderate oxidation stability while overcoming the high viscosity and poor wettability of conventional sulfonyl electrolytes. In addition, the investigation of the steric-hindrance-induced reductive decomposition of DMSF demonstrates that the electron-donating effect of the methyl groups delocalizes the electron density around the nitrogen atom, lowering the LUMO energy level of DMSF and promoting its preferential reduction to form a hybrid LiF/Li2S-rich SEI. As a result, the improvement of the Li metal in terms of cycling is evident in the DMSF electrolyte, where the uniform Li+ deposition significantly suppressed the dendrite growth. In the 50 µm Li‖LiNi0.8Co0.1Mn0.1O2 (NCM811) cell, stable cycling over 850 cycles (80% retention) at 4.5 V is achieved by using DMSF-electrolyte. This cell also delivers a specific capacity of 2.0 and 3.6 mAh at −50 and 60 °C (vs. 3.5 mAh at 25 °C), respectively, and could reversibly operate for 100 cycles. To validate the application of DMSF, a 5 Ah Li‖NCM811 pouch cell is assembled and showcases a competitive performance containing an energy density of 540 Wh kg−1 with 83.2% capacity retention after 110 cycles.
To validate the above strategy, N,N-dimethylsulfamoyl fluoride (DMSF) was designed as a functional sulfonyl solvent for the LMB electrolyte. DMSF was synthesized via a nucleophilic substitution reaction, in which dimethylsulfamoyl chloride was reacted with antimony trifluoride at 60 °C for 24 h under stirring, followed by distillation and purification. As controls, sulfamoyl fluoride (SF) and trifluoromethyl-substituted sulfonamide (DMSTF) were prepared to investigate the effect of –CH3 and –CF3 groups on DMSF. (Fig. S2, detailed procedures are provided in the Experimental section). To balance ionic conductivity and cost, the electrolyte was formulated with LiFSI, LiPF6, and DMSF at a molar ratio of 1
:
0.1
:
5 (1.6 mol L−1). The LiPF6 additive helps form a stable passivation film on the surface of aluminum foil, improving the stability of the cathode during cycling at a high charge cut-off voltage. The electrolytes based on DMSF, SF, and DMSTF are denoted as FSI/PF-DMSF, FSI/PF-SF, and FSI/PF-DMSTF, respectively.
The reduction behavior of each electrolyte was studied in the Li‖Cu half-cell by cyclic voltammetry (CV) measurement. The result reveals that the methylation of the α-H atom in DMSF significantly suppressed the reduction current (Fig. 2b). Previous research indicates that the α-H of electrolytes is one of the culprits of unstable LMB cycling. When Li metal comes into contact with FSI/PF-SF containing α-H, a violent reductive decomposition occurs, while the Li metal immersed in FSI/PF-DMSF was stable (Fig. S4). More importantly, compared to SF, the steric hindrance effect resulting from the dimethyl group facilitates the dispersion of electronic clouds on DMSF (2.43 V) by delocalizing the electron density around the nitrogen atom, leading to a higher reduction potential. The calculation of electrostatic distribution and the lowest unoccupied molecular orbital (LUMO) energy levels (Fig. S3 and S5) also confirms the above result. Therefore, it is inferred that a stable SEI can be quickly formed on the Li metal surface through the prior reduction of DMSF, thereby restraining the severe reduction of electrolytes at low potential (high energy).
The ionic conductivity of the electrolyte was evaluated at different temperatures. Compared to FSI/PF-DMSTF, a higher ionic conductivity was achieved by FSI/PF-DMSF and FSI/PF-SF (Fig. 2c), which demonstrates that the large molecular size caused by methylation has a lower impact on ion transport of the electrolyte compared to –CF3 substitution. In general, the hydrogen (H) bonding between SF is a key factor leading to a decrease in conductivity. For DMSF, despite the H-bonding effect being reduced, it has a larger molecular size than SF. Therefore, under the combined influence of these two factors, FSI/PF-DMSF and FSI/PF-SF exhibit similar ionic conductivity. However, the –CF3 substitution further increases the solvent size of DMSTF, breaking the balance between molecular size and H-bonding effect in DMSF. Thus, FSI/PF-DMSTF shows the lowest ionic conductivity among the studied electrolytes. Besides, the ionic conductivity of FSI/PF-DMSF is 4.8, 3.3, 2.3, 1.5, and 0.12 mS cm−1 at 25, 0, −20, −40, and −50 °C, respectively. In view of the room-temperature ionic conductivity of the local high-concentration electrolyte (LHCE, Li salt concentration: 1–1.5 M), located at 1–2 mS cm−1, FSI/PF-DMSF shows potential to enable the cell with stable operation across a wide temperature range. It should be mentioned that FSI/PF-DMSF retains the non-flammable properties of the sulfonyl-based electrolyte (Fig. S6).
The solvation structure of FSI/PF-DMSF was investigated using Raman and nuclear magnetic resonance (NMR) spectra. As shown in Fig. 2d, the S–N–S stretching vibration mode of the FSI− anion is observed in the 680–800 cm−1 frequency range.37,38 The spectra were deconvoluted to peaks centered at ∼726, 732, 746, and 759 cm−1, respectively, for assigning to the solvent-separated ion pair (SSIP), contact ion pair (CIP), and aggregate (AGG).35 The fraction of the SSIP decreases from 49.8% (1
:
7) to 34.6% (1
:
3), whereas the fraction of the AGG increases from 31.6 (1
:
7) to 50.3% (1
:
3) (Fig. 2e). The obvious change in the proportion of each solvation cluster is indicative of the effective regulation by the solvent. Compared to SF (Fig. S7), the 1
:
5-type electrolyte using DMSF contains more AGG clusters (43.4%), demonstrating the weak interaction between DMSF and Li ion. In addition, a free DMSF molecule exhibits a stretching vibration band at 1195 cm−1. This band shifts up to 1229 cm−1 when DMSF participates in Li+ solvation. 1H nuclear magnetic resonance (NMR) spectroscopy was further conducted and shows that the downfield shift in the proton signal of DMSF in FSI/PF-DMSF (0.06 ppm) is noticeably smaller than that in the case of SF in FSI/PF-SF (0.11 ppm) (Fig. 2f), validating the weak DMSF–Li+ binding. Moreover, according to the molecular dynamics (MD) simulations, the calculated coordination numbers (CNs) between Li+ and oxygen atoms of DMSF (O_DMSF) and FSI− (O_FSI−) were approximately 3.2 and 2.3, respectively. For the SF system, the CN is 3.7 and 1.7, respectively, for the O_SF and O_FSI− (Fig. S8). The weak DMSF–Li+ binding could be attributed to the methylation of the nitrogen atom, in which the introduction of –CH3 enhances the steric hindrance effect of DMSF, weakening the coordination of the sulfonyl group with Li ions.
Galvanostatic rate tests were conducted to evaluate the dendrite-suppressing effect of FSI/PF-DMSF as the current density increased from 0.5 to 10.0 mA cm−2. As shown in Fig. 3b, FSI/PF-DMSF enables stable Li plating/stripping behavior in Li symmetric cells even at 10.0 mA cm−2, while the LiFSI-1.1DME cell exhibits significant voltage fluctuations, especially at high rates. As the current density increases from 0.5 to 10 mA cm−2, the overpotential of Li nucleation in FSI/PF-DMSF changed from 56.5 and 261.4 mV (Fig. 3c and S9). By contrast, the overpotential increase is significant in LiFSI-1.1DME under the same conditions, from 65.0 to 559.4 mV. The galvanostatic cycling performance of the Li metal anode was also improved by using FSI/PF-DMSF (Fig. 3d). The symmetric cell with FSI/PF-DMSF maintains a minimal voltage polarization of 22.9 mV after 600 hours of cycling at 0.5 mA cm−2. However, the polarization of the LiFSI-1.1DME cell is twice that of the FSI/PF-DMSF cell in the initial cycle and gradually decreases over the following cycles (0–200 hours). This long-term process of voltage variation largely corresponds to an increase in the active interface area caused by Li cycling (Fig. S10). For the same reason, the stable voltage fluctuation of the FSI/PF-DMSF cell throughout the cycles is indicative of the effective suppression of dendrite growth and interface degeneration.
To further investigate the compatibility of FSI/PF-DMSF with Li metal, the Li plating/stripping reversibility was evaluated using Li‖Cu half cells at 1 mA cm−2 with 2 mAh cm−2 Li capacity. As shown in Fig. 3e, both electrolytes exhibit an initial coulombic efficiency (CE) of >92%. For LiFSI-1.1DME, the CE remains stable during the initial 300 cycles, followed by significant fluctuations, indicating that interface damage gradually accumulates with cycling and severely affects electrochemical behavior once a threshold is reached.
Consistent with the results of Li symmetric cells, FSI/PF-DMSF demonstrates improved Li metal compatibility, achieving an average CE of 99.55%. This advantage of FSI/PF-DMSF was more pronounced at higher current densities (Fig. S11).
The morphology of deposited Li was examined using scanning electron microscopy (SEM) and cryogenic-focused ion beam (cryo-FIB) techniques. As shown in Fig. 3f, g and S11, the Li deposited after 5 cycles exhibits bulk, dense, and dendrite-free morphologies in both FSI/PF-DMSF and LiFSI-1.1DME. Notably, the primary particle size obtained from FSI/PF-DMSF is significantly larger than that produced in LiFSI-1.1DME. This is because the low overpotential in FSI/PF-DMSF is beneficial for reducing nucleation sites, promoting the Li deposition layer with a morphology featuring low specific surface area. From the cross-sectional view, the Li deposition in FSI/PF-DMSF exhibits greater compactness than that in LiFSI-1.1DME, where the density of the boundary layer formed at the contact interface of the primary Li deposition particle is higher in LiFSI-1.1DME than in FSI/PF-DMSF. The boundary originates from the SEI, which has anisotropy with Li metal and reduces the electronic conductivity of the Li deposition layer to some extent. Therefore, compared to LiFSI-1.1DME, the Li plating/stripping in FSI/PF-DMSF shows higher stability and reversibility (Fig. S12 and S13), even though there is no obvious formation of Li dendrites in either system.
Notably, in the S 2p spectra, inorganic sulfur-containing components in the SEI of FSI/PF-DMSF are distinct from those generated by the reduction of FSI− in LiFSI-1.1DME (Fig. 4b). The sulfur-containing inorganic components in FSI/PF-DMSF are single, with only Li2S signals detected. In contrast, the SEI of LiFSI-1.1DME shows diverse reduction products of FSI− anions and presents a mosaic structure (Fig. S16). These results indicate that the Li2S formed in FSI/PF-DMSF is derived from the decomposition of DMSF rather than FSI−, which is in line with the CV observation that DMSF has a high reduction potential and could preferentially passivate the Li metal anode to reduce the decomposition of anions.
The ab initio molecular dynamics (AIMD) simulation was conducted to elucidate the decomposition process of FSI/PF-DMSF on the Li metal surface (Fig. 4c). In the initial stage (60 fs), the DMSF molecule adsorbs onto the Li metal surface and then undergoes reduction, decomposition, and de-fluorination, forming LiF on the Li metal surface (280 fs). Between 280 and 670 fs, the (CH3)N–SO2− group moves closer to the Li metal interface and cleaves into (CH3)N− and SO2− fragments. By 710 fs, SO2− further decomposes, resulting in the formation of Li2S on the Li metal surface. As shown in Fig. 4d, the reduction of FSI/PF-DMSF mainly involves the de-fluorination and de-sulfurization of the DMSF molecule, while the FSI− anion is less participating in these reactions as a result of the calculation. This further indicates the preferential decomposition behavior of DMSF. Combined with the XPS results, it can be confirmed that methylation promotes the decomposition of DMSF, forming a stratified organic–inorganic SEI with a rich LiF/Li2S inner layer to effectively facilitate the interfacial Li-ion kinetics and enable uniform Li deposition with large size.
The temperature range for the operation of the FSI/PF-DMSF cell was also investigated as shown in Fig. 5c. As expected, 3.6 mAh of the initial capacity is output at 60 °C, and this cell also shows a capacity retention of 85.0% after 100 cycles. This high-temperature performance of the cell could be attributed to the stable chemical structure of DMSF and the SEI. At low temperature, the Li‖NCM811 cell with FSI/PF-DMSF shows a capacity retention of 85.6% at −20 °C compared to the reversible capacity derived at 25 °C. Meanwhile, the cycling remains stable without any significant capacity decline. In addition, when the cell is tested at −50 °C, a reversible capacity of around 1.8 mAh was achieved (51.4% of the 25 °C-capacity output), and this cell can stably operate over 100 cycles (Fig. S20). Obviously, the weak desolvation barrier stemmed from the steric hindrance effect of DMSF ensures favorable Li-ion kinetics at low temperatures. The SEI induced by FSI/PF-DMSF, in addition, could promote the interfacial Li-ion transport and stabilize the Li metal interface when cycled at low temperatures. Therefore, FSI/PF-DMSF enables the cell to operate over a wide temperature range of −50 to 60 °C.
Given that the improved performance of the FSI/PF-DMSF cell at low temperature arises from the enhanced kinetics imparted by DMSF, the fast-charging cycling of the cell with FSI/PF-DMSF is also worth investigating. As shown in Fig. 5d and S21, although polarization is increased, the Li‖NCM811 cell with FSI/PF-DMSF still delivers a capacity of 2.0 mAh (135.5 mAh g−1) at 5C. Moreover, 83.2% of the reversible capacity was retained after 150 cycles at 5C, with an average CE of 99.77% (Fig. S22), demonstrating the versatility of the electrolyte by using DMSF, including high voltage, wide operating temperature range, and fast charging.
Furthermore, an industrial-level evaluation of FSI/PF-DMSF was performed by testing 5 Ah Li‖NCM811 pouch cells. From the result shown in Fig. 5f, this pouch cell attains an energy density of 540 Wh kg−1 based on total cell weight (Table S2), meeting the targets outlined by the U.S. Battery500 project. The cell also maintained over 83% capacity retention throughout 110 cycles, with only a marginal increase in polarization observed during continuous cycling, which can also support pouch cell cycling at 2C (Fig. S23). Notably, PTE-PE-SPE also provides high-safety performance for the high-energy LMBs. As shown in Fig. S24, the fully charged (4.5 V, after cycling) Li‖NCM811 pouch cell did not catch fire during a nail penetration process. Under the benchmark conditions of energy density ≥300 Wh kg−1 and cycle life ≥100 cycles, this 5 Ah pouch cell shows an obvious advantage by using FSI/PF-DMSF, outperforming the Li metal batteries reported in the related literature (Fig. 5g and Table S3).
Footnote |
| † These authors contributed equally to this work. |
| This journal is © The Royal Society of Chemistry 2026 |