Changde
Ma
a,
Pratteek
Das
a,
Xiaoyu
Shi
a,
Feng
Zhou
a and
Zhong-Shuai
Wu
*ab
aState Key Laboratory of Catalysis, Dalian Institute of Chemical Physics, Chinese Academy of Sciences, 457 Zhongshan Road, Dalian 116023, China. E-mail: wuzs@dicp.ac.cn
bDalian National Laboratory for Clean Energy, Chinese Academy of Sciences, 457 Zhongshan Road, Dalian 116023, China
First published on 15th July 2025
Supercapacitors are critical for high-power applications due to their fast charge–discharge capabilities and long lifespans. However, achieving high performance at ultra-low temperatures remains a significant challenge, limiting their use in extreme environments. The electrolyte responsible for ion transport is the key factor governing the low-temperature performance of supercapacitors. In this perspective, we focus on the recent advances in low-temperature electrolytes for supercapacitors. We first introduce the critical physical parameters for evaluating low-temperature electrolytes. Then, we emphasize the key design strategies for low-temperature electrolytes, followed by a detailed discussion of their anti-freezing mechanisms, encompassing aqueous, organic, ionic liquid, and gel-based electrolytes. Additionally, particular emphasis is placed on the theoretical simulation and advanced characterization techniques, given their capability to elucidate the microscopic structure of the electrolyte and provide comprehensive insights into its energy storage mechanism. Finally, we have provided an outlook on the current challenges and future development directions of low-temperature electrolytes, which is expected to offer promising strategies for reliable, high-performance supercapacitors in ultra-low temperature applications.
The electrolyte, responsible for ion transport, is the key factor determining the supercapacitors' low-temperature capabilities. However, conventional electrolytes, with their high freezing points and slow ion transport kinetics, limit the applications of supercapacitors in low-temperature environments. Specifically, at low temperature, the sluggish ion migration in the bulk electrolyte results in an increased impedance; meanwhile, the increase in viscosity triggers severe concentration polarization. Furthermore, there is an obstruction to ion diffusion at the electrode/electrolyte interface, resulting in a significantly increased charge transfer impedance.9 These factors result in severe capacitance decay. To overcome these challenges, it is essential to develop electrolytes that not only decrease the freezing point but also exhibit other crucial characteristics, including superior ionic conductivity, low viscosity, and excellent chemical stability at low temperature.
In this perspective, we first provide a comprehensive discussion on the intrinsic physical properties of low-temperature electrolytes. Subsequently, we summarize the key strategies reported to address the related challenges, focusing on aqueous, non-aqueous and gel electrolytes. Afterwards, theoretical simulations and advanced characterization techniques are briefly outlined to better analyze the underlying energy storage mechanism at low temperatures (Fig. 1). Finally, strategic research directions for further development are proposed, offering rational guidance and new insight for designing low-temperature electrolytes towards high-performance supercapacitors.
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Fig. 1 Schematic illustration of the main contents for low-temperature electrolytes of supercapacitors. |
To ensure the optimal performance of supercapacitors at low temperatures, the primary consideration is to prevent the electrolyte from freezing. This puts the emphasis on depressing the freezing point to ensure rapid ion movement in electrolyte. For instance, aqueous electrolytes typically have a higher freezing point due to the presence of extensive hydrogen bonding between water molecules. The cryogenic phase transition arises from thermodynamically dominant hydrogen-bond networks that surpass the thermal motion of water molecules at reduced temperatures, inducing spontaneous molecular reorganization into hexagonal crystalline lattices through enthalpy-driven nucleation processes. Therefore, weakening these hydrogen bonds is an effective strategy to extend the operating temperature. In contrast, non-aqueous electrolytes have a lower freezing point, but they also suffer from the issue of significant increase in intermolecular forces, or even freezing at temperatures below −40 °C. For extreme low-temperature applications, it is crucial to carefully design the electrolyte with low freezing point by disrupting the strong interactions between the solvents.
Viscosity (η), as a parameter that describes a liquid's resistance to flow, is closely linked to ion transport behavior. Both ionic conductivity and the diffusion coefficient are affected by viscosity. Higher viscosity generally corresponds to lower ionic conductivity and a smaller diffusion coefficient. Additionally, the wetting properties of the separator and electrode materials are also influenced, with high-viscosity electrolytes typically wetting slower than low-viscosity ones.14 Therefore, the viscosity of the electrolyte significantly impacts the performance of supercapacitors. The exponential relationship (η = η0e−Eb/αKBT) illustrates that even a slight decrease in temperature can cause notable variations in viscosity.8 As a result, high-performance electrolytes that work well at room temperature often have subpar performance at low temperatures owing to increased viscosity. Generally, the viscosity of an electrolyte is determined by the type and concentration of the solvent and salt. Compared to pure solvents, mixed solvents are more commonly employed in low-temperature electrolytes due to the introduction of low-viscosity organic solvents.15 In addition to the solvent, the salt also affects the electrolyte's viscosity. Generally, the coulombic interactions between cations and anions are stronger than the dipole–dipole interactions between solvent molecules, resulting in an increase in viscosity. Moreover, high salt concentration results in the formation of ion pairs or aggregates, and the presence of these aggregates increases the internal friction of the solution. Meanwhile, the interactions between ions (such as electrostatic forces) are enhanced, inducing an increase in viscosity.16
The ionic conductivity (σ) of an electrolyte influences the equivalent series resistance of supercapacitors, which in turn affects the rate performance and power density. Ionic conductivity is primarily dependent on the free-moving ions in the solution. As the temperature decreases, ionic conductivity typically decreases gradually at first and then more sharply below the freezing point. This is attributed to ion aggregation or salt precipitation occurring at lower temperatures, which reduces the number of free-moving ions in the solution, thereby affecting the ionic conductivity. Additionally, ionic conductivity is influenced by the concentration of the electrolyte. It generally increases as ion concentration rises. However, at relatively high concentrations, stronger ion interactions may occur and reduces the number of free-moving ions, potentially resulting in a reduction in conductivity. In addition to temperature and ion concentration, the nature of the charge carriers also plays a significant role in determining ionic conductivity. For instance, solvated cations with smaller solvated radii tend to exhibit high ionic conductivity.
The electrochemical stability window defines the voltage range in which the electrolyte remains stable and does not decompose. In general, electrochemical stability window is largely determined by the highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) energy levels of solvents.17 However, Peljo et al. suggested that the concept of HOMO and LUMO, originally derived from studies on the electronic properties of isolated molecules, may not be directly applicable to complex electrolytes.18 As a result, the redox reactions of multi-component electrolytes cannot be solely evaluated from the HOMO–LUMO energy gap. It has been suggested that the electrochemical stability of electrolytes should be more accurately described by considering oxidation and reduction potentials instead. At low temperatures, the electrochemical stability window of electrolytes can be significantly affected due to changes in the electrolyte's physical and chemical properties. In some cases, at lower temperatures, solvent decomposition is inhibited by slowing down side reactions at the interface, thus elevating the electrolyte's electrochemical stability windows.19
In short, the physical parameters of electrolytes are crucial for the design and performance improvement of low-temperature supercapacitors. To design high-performance electrolytes, it is essential to consider not only individual parameters but also the balance between various factors. Based on the above, diverse strategies have been employed to design various types of low-temperature electrolytes, including aqueous, organic, ionic liquid, and gel electrolytes. A comprehensive analysis of each strategy, along with its corresponding anti-freezing mechanisms, will be systematically discussed in the subsequent sections (Fig. 2).
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Fig. 2 The key design strategies for developing different low-temperature electrolytes for supercapacitors. |
Electrolyte | Concentration | Ionic conductivity [mS cm−1] | Specific capacitance/capacity | Operating temperature [°C] | Electrode material (device type) | Voltage [V] | Ref. |
---|---|---|---|---|---|---|---|
a VHCF: Prussian blue analog, SCs: supercapacitors, AC: activated carbon. | |||||||
CaCl2 in H2O | 3.8 m | 10.1 (−50 °C) | 59.3 F g−1 (0.5 A g−1, 25 °C) | −50 | AC (SCs) | 1.8 | 25 |
Zn(OTf)2 in H2O/ACN | 2 M | 54.2 (25 °C) | 64 mF cm−2 (500 mV s−1, −40 °C) | −40 | MXene@CC//Zn (ZHSs) | 1.6 | 26 |
Ca(ClO4)2 in H2O/ACN | 4.2 m | 1.5 (−50 °C) | 46 F g−1 (1 A g−1, −50 °C) | −50 | AC (SCs) | 2.3 | 22 |
CaCl2 in EG/H2O | 3.86 m | 0.69 (−50 °C) | 18.4 mF cm−2 (0.1 mA cm−2, 20 °C) | −40 | AC (SCs) | 1.6 | 27 |
LiTFSI in H2O | 5 m | 50 (RT) | 22 F g−1 (10 A g−1, 15 °C) | −30 | AC (SCs) | 2 | 13 |
LiTFSI in ACN/H2O | 5 m | 17.4 (25 °C) | 8.6 F g−1 (10 A g−1, −30 °C) | −30 | AC (SCs) | 2.2 | 28 |
LiNO3 in H2O/1,3-propylene glycol | 3.65 m | 67.5 (25 °C) | 20.6 F g−1 (5 mV![]() |
−40 | AC (SCs) | 2.0 | 20 |
3NaClO4–2CO(NH2)2/H2O | — | 135 (25 °C) | 22.6 F g−1 (20 mV![]() |
−40 | AC (SCs) | 2.25 | 29 |
5.3 (−50 °C) | |||||||
CsAc in H2O | 10 m | 0.8 (−80![]() |
200 mF cm−2 (0.1 mA![]() |
−95 | AC (SCs) | 0.8 | 30 |
H2SO4–ZnCl2 acid-salt hybrid electrolyte | 0.2–5.4 M | 6.97 (−60 °C) | 39.8 mA h g−1 (1 A g−1, −80 °C) | −80 | VHCF//α-MoO3 (hybrid capacitors) | 1.5 | 31 |
Anti-freezing additives are typically selected for their capacity to establish strong coordination or hydrogen bonds with water molecules, as well as their high solubility in water. The most-commonly reported anti-freezing additives include inorganic salts and certain organic co-solvents, like ethylene glycol (EG), acetonitrile (ACN), and glycerol.10 For example, considerable research has focused on incorporating calcium chloride (CaCl2) into aqueous electrolytes to improve their antifreeze properties.32,33 The intense interaction between CaCl2 and water molecules disrupts the original hydrogen bonding framework, leading to a lower freezing point and an expanded operating voltage. As a typical example, You and co-workers developed a CaCl2-based brine refrigerant electrolyte (BRE) for supercapacitors, featuring a significantly reduced freezing point (−55 °C) and sustaining high ionic conductivity (10.1 mS cm−1) even at −50 °C. This electrolyte enables the supercapacitors to retain 80% of their room-temperature capacitance at −50 °C while demonstrating superior cycle life and outstanding capacitance retention (Fig. 3a–c).25 Furthermore, organic co-solvents with strong water-coordinating capabilities or low freezing points have been introduced into aqueous electrolytes to disrupt the hydrogen bonding, effectively suppressing the freezing of the aqueous solution. For example, Liu et al. employed ACN as a low-temperature co-solvent to modify the aqueous electrolyte. The ACN additive disrupted hydrogen bonding between water molecules and restructured the Zn2+ solvation sheath, thereby reducing ion transfer resistance and enabling highly reversible Zn/Zn2+ redox chemistry. Consequently, the Zn-ion hybrid supercapacitor delivered an area-specific capacitance of 64.0 mF cm−2 at 500 mV s−1 (−40 °C) and exhibited long-term cyclability (Fig. 3d–g).26 In addition, several studies have explored the use of both inorganic salts and organic solvents as additives to create low-temperature electrolytes. As exemplified, Yang et al. proposed a cost-efficient hybrid electrolyte for low-temperature micro-supercapacitors (MSCs) by incorporating CaCl2 and EG. The addition of CaCl2 decreases the quantity of water molecules involved in strong hydrogen bonding, while EG further minimizes the water molecules in the primary solvation shell. This combination yields an electrolyte that exhibits a high voltage stability of 3.5 V and an extremely low freezing point of −120 °C. Consequently, the MSCs retain 62% capacitance at −40 °C compared to their room-temperature performance.27
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Fig. 3 Low-temperature aqueous electrolytes engineered by utilizing inorganic salts (e.g., CaCl2) or organic solvents (e.g., ACN) as antifreeze additives. (a) Digital photos of the BREs and control electrolytes. (b) Variation in ionic conductivity of the BREs with temperature. (c) Change in capacitance of the supercapacitor at 1 A g−1 with a gradual decrease in temperature from 25 °C to −50 °C. Reproduced with permission.25 Copyright 2023, Wiley-VCH. (d) Schematic illustration of Zn2+ solvent sheath in Zn(OTf)2 electrolyte (left) and Zn(OTf)2 + ACN electrolyte (right). (e) Photograph of the two types of electrolytes at −40 °C. (f) The capacitance of supercapacitors using the two types of electrolytes at varying temperatures, with pink representing the electrolyte containing ACN. (g) The contact angle between the Zn anode and different electrolytes. Reproduced with permission.26 Copyright 2025, Royal Society of Chemistry. |
The WIS electrolytes have experienced rapid development in electrochemical energy storage devices, following their initial proposal by Suo et al. in 2015.34 Recently, WIS electrolytes have demonstrated great potential for use in supercapacitors, owing to their wide electrochemical stability window and excellent ion transport properties.16,21,35 Generally, the added salt forms hydrated ions with free water molecules, decreasing the number of hydrogen bonds and thereby lowering the freezing point. By exploiting this property, high-concentration electrolytes have been developed to function as low-temperature electrolytes for supercapacitors. For instance, Zhang and colleagues found that the 5 m LiTFSI/H2O electrolyte exhibits excellent low-temperature behaviors even at −30 °C. They also explored the temperature-related electrochemical properties of electrolytes with different concentrations, analyzing their intermolecular interactions and solvation structures using molecular dynamics simulations and Raman spectroscopy (Fig. 4a–d).13 However, it is noted that as the salt concentration increases to a higher level, salt crystallization is likely to occur at low temperatures, leading to performance decline or potential failure of supercapacitors. This issue can be effectively mitigated by incorporating organic solvents into the high-concentration electrolyte. As a representative example, Dou et al. developed a co-solvent-in-salt system by introducing ACN into a 21 m LiTFSI/H2O electrolyte, creating an ACN/WIS electrolyte (AWIS). This work demonstrates that combining highly concentrated aqueous electrolytes with organic solvents is a promising strategy for high-performance supercapacitors with both a high voltage and wide temperature range (Fig. 4e–g).28
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Fig. 4 Design strategy for low-temperature aqueous electrolytes based on WIS electrolytes. (a) The left panel illustrates structural models of LiTFSI/H2O systems at three distinct concentrations, while the right panel depicts the correlation between water's hydrogen-bonding configurations and their corresponding Raman spectral features. (b) Raman spectral analysis of the O–H stretching region in 5 m LiTFSI/H2O systems across varying temperatures. (c) Diffusion coefficients of Li+ ions at various temperatures. (d) Evaluation of temperature-dependent specific capacitance in supercapacitors employing 5 m LiTFSI aqueous electrolytes. Reproduced with permission.13 Copyright 2023, Elsevier. (e) Images illustrating the preparation of AWIS electrolytes with various concentrations. (f) Influence of electrolyte concentration on ionic conductivity and viscosity. (g) Comparison of the specific capacitance at different current densities. Reproduced with permission.28 Copyright 2018, Royal Society of Chemistry. |
DESs are typically binary or multi-component mixtures composed of a hydrogen bond acceptor and a hydrogen bond donor, with the eutectic point significantly lower than that of its individual components (Fig. 5a).36 Certain aqueous salt hydrate systems, consisting of mixtures of ice and partially dissolved salt hydrates under low-temperature conditions, can also be considered as DESs. The eutectic point of such aqueous solutions can be determined using a solid–liquid phase diagram. Additionally, thermodynamic simulations can be employed to generate phase diagrams for such electrolytes, aiding in the identification of the optimal salt-to-water proportion needed to attain the target freezing point.37 At the “eutectic concentration”, the mixture shows the lowest freezing point.38 In recent years, DESs have garnered significant attention as promising electrolytes for supercapacitors operating at low temperatures. For instance, Ah-Lung et al. proposed an environmentally friendly and cost-effective ternary deep eutectic electrolyte system composed of LiNO3, water, and 1,3-propylene glycol, aiming to design an electrolyte with a broad liquid phase range. When used in supercapacitors, this electrolyte enabled the device to achieve a minimal capacitance loss of only 6% at −20 °C and 29% at −40 °C (Fig. 5b and c).20 As another typical example, Bo et al. put forward a ternary interaction approach involving cations, water, and urea to create electrolytes suitable for low-temperature applications, demonstrating aqueous electrolytes with an exceptionally depressed freezing point and superior ionic conductivity. The optimized ternary aqueous electrolyte achieves an extremely low freezing point of −70 °C and exhibits a remarkable ionic conductivity of 5.3 mS cm−1 at −50 °C. Even at −40 °C, the supercapacitors employing the 13NaClO4–2CO(NH2)2/H2O electrolyte exhibit approximately 70% capacitance retention with the scan rate increasing from 20 to 100 mV s−1, significantly surpassing that of supercapacitors using a 17 m NaClO4 WIS electrolyte (Fig. 5d and e).29
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Fig. 5 DES strategy for low-temperature electrolyte design. (a) Schematic depiction of the eutectic point in a binary phase diagram. Reproduced with permission.36 Copyright 2014, American Chemical Society. (b) Thermal analysis curves of the LiNO3-based eutectic and the eutectic containing 18% 1,3-propylene glycol. (c) Capacitance retention at different temperatures. Reproduced with permission.20 Copyright 2023, Wiley-VCH. (d) Schematic depiction of the proposed ternary aqueous electrolyte. (e) Rate capability of the supercapacitor utilizing the 13NaClO4–2CO(NH2)2/H2O electrolyte at various temperatures. Reproduced with permission.29 Copyright 2024, Elsevier. |
Extending the operational temperature range of aqueous electrolytes has emerged as a significant research focus, with recent advances unveiling novel mechanism insights. For example, entropy regulation of specific electrolyte systems may offer a novel strategy for depressing the freezing point of aqueous solutions. In this context, Qiu et al. proposed the concept of entropy-driven glass-forming liquids (EDGFLs) as an innovative paradigm for designing freeze-resistant electrolytes. Through precise modulation of local structural ordering, the glass-transition temperature (Tg) can be systematically engineered to suppress energy-dominated ice crystallization while facilitating entropy-driven glass transition. This behavior can be fundamentally understood through the competitive interplay between ion pair correlation entropy and water's tetrahedral entropy. Moreover, experimental validation is achieved through differential scanning calorimetry (DSC) and in situ optical microscopy. The resulting EDGFL system, exhibiting an ultralow Tg of −128 °C, enables supercapacitors to facilitate superior capacitance retention under cryogenic conditions while sustaining operational stability down to −95 °C (Fig. 6).30 Furthermore, acid-salt hybrid electrolytes featuring stable anion–cation-H2O solvation structures facilitate unconventional proton conduction at cryogenic temperatures. A representative study by Cui et al. demonstrated that such hybrid electrolytes can effectively reorganize water network channels to promote efficient ion transport, enabling rapid ionic conductivity and superior rate performance at low temperatures. It is revealed from Raman spectroscopy that the hydrogen bond network structure between water molecules is disrupted by Cl− and Zn2+, leading to a depression of the freezing point. While such disruption mitigates solvent crystallization at low temperatures, it is important to note that the strong yet localized hydrogen bonding, particularly between the ions and solvent molecules, can persist within the system. These localized interactions may facilitate the formation of stable solvation structures and continuous ion conduction pathways, which are beneficial for maintaining efficient ion transport under cryogenic conditions. As a result, a reversible capacity of 151 mA h g−1 (46.6% of room-temperature capacity) can be retained at 1 A g−1 even at −60 °C, highlighting the electrolyte's superior low-temperature adaptability (Fig. 7).31
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Fig. 6 Entropy-engineered electrolyte systems for low-temperature supercapacitors. (a) Schematic representation of the phase behavior in a non-equilibrium binary system comprising water and salt. (b) DSC measurements of CsAc aqueous solutions at varying concentrations. (c) Dependence of primary phase transition temperatures on CsAc concentration. (d) In-situ optical microscopy observations of electrolytes during the cooling process. (e) Charge–discharge profiles at different temperatures. (f) Long-term cyclability observed at −95![]() |
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Fig. 7 Acid-salt hybrid electrolytes for low-temperature supercapacitors. (a) Diagram of the structure evolutions for designing low-temperature electrolytes. (b) The DSC curves of different electrolytes. (c) The Raman spectra of different electrolytes. (d) The fitted O–H stretching vibration in 0.2–5.4 m electrolyte. (e) The proportion of strong, weak, and non H-bonds in different solutions. (f) The specific discharge capacity at various current densities and temperatures. Reproduced with permission.31 Copyright 2024, Wiley-VCH. |
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Fig. 8 Design of a low-temperature organic electrolyte via co-solvent formulation or novel salt engineering. (a) Schematic depiction of SC behavior at various temperatures. (b) CV curves of supercapacitors from 20 to −100 °C (c) CV curves measured at −100 °C with different scan rates. Reproduced with permission.15 Copyright 2019, Elsevier. (d) Molecular structures of the electrolyte components. (e) Ionic conductivities of SBP-FSI/PC based electrolytes and TEA-BF4/PC commercial electrolytes at different temperatures. (f) The rate capability of supercapacitors based on these two electrolytes. Reproduced with permission.40 Copyright 2019, Elsevier. |
Apart from the solvent, novel salts with excellent solubility, high ionic conductivity, and superior electrochemical stability, such as spiro-(1,1′)-bipyrrolidinium bis(fluorosulfonyl)imide (SBP-FSI), have been progressively developed for organic electrolytes.40–42 Electrochemical characteristics of the electrolyte are largely determined by the specific types of ions present in the salt. In comparison to the commercially available electrolyte salt (TEABF4), SBP-FSI exhibits superior performance at low temperatures. Moreover, SBP+ also has a smaller molecular volume and a shorter distance between the ion center and electrode surface, thereby contributing to a higher theoretical specific capacitance. For instance, Zhang et al. demonstrated that the combination of SBP-FSI and propylene carbonate (PC) displays greater ionic conductivity at low temperatures for supercapacitors compared to TEA-BF4/PC. As a result, SBP-FSI/PC based supercapacitors showed excellent rate capabilities at low temperature, exhibiting 64.8% capacitance retention versus TEA-BF4/PC's near-complete performance collapse (90% reduction) under 5 A g−1 at −40 °C (Fig. 8d–f).40
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Fig. 9 Low-temperature ionic liquid electrolytes developed through eutectic composition or organic co-solvent strategies. (a) Employing a eutectic ionic liquid mixture enables supercapacitor operation at temperatures as low as −50 °C. (b) DSC thermograms of (I) PIP13FSI, (II) PYR14FSI and (III) (PIP13FSI)0.5(PYR14FSI)0.5 mixture, along with their molecular structures. (c) CV curves measured in the ionic liquid mixture electrolyte at low temperatures. Reproduced with permission.46 Copyright 2011, American Chemical Society. (d) Physical characteristics of the electrolyte components. (e) DSC curves of different electrolytes. (f) GCD profiles of P-AN, P-AN-PC, and P-AN-MB (AN: ACN) electrolyte-based supercapacitor at −70 °C. Reproduced with permission.47 Copyright 2022, Royal Society of Chemistry. |
Furthermore, incorporating low-freezing-point, low-viscosity organic solvents into ionic liquids presents an effective approach to lowering the freezing point and enhancing ionic conductivity. This enhancement in ionic conductivity results from reduced ion association in ionic liquid-based electrolytes upon solvation by added solvents, which lowers the viscosity and increases ionic mobility. Ideally, organic solvents should be selected to disrupt ion pairing in ionic liquids while minimizing the formation of strongly solvated ion species, thus ensuring high ion mobility. For example, Tang et al. demonstrated that incorporating mixed solvents, such as ACN and methyl butyrate (MB), into ionic liquids significantly enhances their low-temperature performance. By combining spectroscopic characterization with theoretical calculations, it was shown that the unique solvation interactions between the ionic liquid and solvents significantly reduce the electrostatic forces between the cations and anions as well as the hydrogen bonding between them (Fig. 9d–f).47 However, it is important to note that while adding organic solvents into ionic liquids is an efficient strategy for reducing the freezing point, it can also narrow the electrochemical stability window simultaneously. Therefore, the balance between the operating temperature and working voltage needs to be considered. Representative low-temperature organic and ionic liquid electrolytes are summarized in Table 2.
Electrolyte | Concentration | Ionic conductivity [mS cm−1] | Specific capacitance | Operating temperature [°C] | Electrode material (device type) | Voltage [V] | Ref. | |
---|---|---|---|---|---|---|---|---|
Organic electrolytes | MeEt3NBF4 in ACN/DIOX. | 0.5 M | 18.5 (20 °C) | 164 F g−1 (5 mV s−1, −100 °C) | −100 | AC (SCs) | 2.5 | 15 |
SBP-FSI in PC | 1 M | 17.4 (20 °C) | 70 F g−1 (5 A g−1, −40 °C) | −40 | AC (SCs) | 2.7 | 40 | |
EMI-TFSI in multiple organic solvents | 1 M | 3.9 (−50![]() |
39.1 F g−1 (5 A g−1, RT) | −50 | AC (SCs) | 3 | 39 | |
SBPBF4 in ACN/MF | 0.3 M | — | 157 F g−1 (100 mV s−1, −100 °C) | −100 | AC (SCs) | 2.5 | 48 | |
[EMIM][BF4] in ACN/MA | 1 M | — | 45 F g−1 (0.5 A g−1, RT) | −100 | AC (SCs) | 3.5 | 19 | |
Ionic liquid electrolytes | (PIP13FSI)0.5(PYR14FSI)0.5 | 1![]() ![]() |
4.9 (20 °C) | — | −50 | CNTs (SCs) | 3.7 | 46 |
[Pyrr][NO3] [Pyrr][TFSI] | 0.72![]() ![]() |
1 (−10 °C) | 209 F g−1 (5 mV s−1, 25 °C) | −60 | AC (SCs) | 2.5 | 49 | |
PMImNTf2 in ACN/MB | 1![]() ![]() ![]() ![]() |
2.46 (−70 °C) | 18.6 F g−1 (0.5 A g−1, −50 °C) | −70 | AC, (SCs) | 2.8 | 47 |
Electrolyte | Conductivity [mS cm−1] | Specific capacitance/capacity | Operating temperature [°C] | Electrode material (applied device) | Voltage [V] | Ref. |
---|---|---|---|---|---|---|
a NMP: N-methylpyrrolidone. | ||||||
LiOTf in PVA/NMP | 1.34 (−25 °C) | 25.4 mF cm−2 (1 mA cm−2, 25 °C) | −40 | CNT (SCs) | 2.5 | 56 |
10.65 (25 °C) | ||||||
NaAc in hydrogel | — | 205.9 F g−1 (0.2 A g−1, 20 °C) | −40 | AC (SCs) | 2 | 57 |
LiBr in poly (ionic liquid) hydrogel | 26 (25 °C) | 163 mF cm−2 (1 mA cm−2, −20 °C) | −20 | AC (SCs) | 1 | 50 |
Lignin based hydrogel | 96 (RT) | 150 F g−1 (1 A g−1, −30 °C) | −30 | AC (SCs) | 1 | 58 |
H2SO4 in zwitterionic hydrogel | 1.51 (−50 °C) | 62.0 F g−1 (62.5 mA g−1, −50 °C) | −50 | AC (SCs) | 1 | 59 |
ZnSO4 in hydrogel | 7.68 (25 °C) | 82.14 F g−1 (0.5 A g−1, 25 °C) | −20 | AC (SCs) | 1.4 | 60 |
CuSO4 in PVA | 0.179 (−15 °C) | 72.62 F g−1 (100 mA g−1, 25 °C) | −80 | Graphene (SCs) | 1 | 61 |
ZnSO4 in hydrogel electrolyte | 24.3 (−20 °C) | 117.5 mA h g−1 (0.25 A g−1, −20 °C) | −20 | AC//Zn (ZHSs) | 1.8 | 62 |
Zn(OTf)2 in PVA gel | — | 49.1 mA h g−1 (5 A g−1, 25 °C) | −30 | MXene//Zn (ZHSs) | 1.2 | 63 |
Designing an anti-freezing hydrogel electrolyte involves optimizing several factors to ensure that the hydrogel not only retains its ionic conductivity at low temperatures but also its mechanical stability. In general, the strong hydrogen bonding between water molecules is a major challenge in developing anti-freezing hydrogel electrolytes. To address this, organic solvents are often incorporated into hydrogel electrolytes to disrupt the hydrogen-bonding network of water molecules, effectively suppressing the freezing behavior of the hydrogel electrolyte. For instance, Wang et al. proposed the development of anti-freezing hydrogel electrolytes with enhanced water deactivation by incorporating N-methylpyrrolidone solvent. As a result, the flexible supercapacitors exhibit nearly rectangular CV curves and symmetrical triangular GCD profiles within the temperature range of −40 to 0 °C. The flexible supercapacitors deliver a record areal energy density of >13.55 μ Wh cm−2 with voltage outputs exceeding 2.5 V across −40 to 25 °C. The environmental temperature fluctuation test indicates that the device exhibits excellent environmental adaptability (Fig. 10).56 While incorporating organic solvents effectively lowers the freezing point, the mechanical strength of hydrogels remains unsatisfactory owing to the insufficient interactions between polymer chains.64 To address this issue, a solution can be found by designing and synthesizing dual-crosslinked hydrogels incorporating ethylene glycol-functionalized groups.65
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Fig. 10 Anti-freezing hydrogel electrolytes designed by introducing organic solvents. (a) Preparation process of the gel electrolyte. (b) Tensile stress–strain curves at 25 and −25 °C of the gel electrolyte. (c) CV curves and (d) GCD profiles of supercapacitors from 25 to −40 °C. (e) Specific capacitance and energy density of supercapacitors at different temperatures. (f) Continuous reversible changes of capacitance retention of supercapacitors under various temperature conditions. Reproduced with permission.56 Copyright 2025, Wiley-VCH. |
The addition of salts can also significantly inhibit the freezing behavior of hydrogel electrolytes.57,61,66–68 In general, introducing salt into the system disrupts both inter- and intra-chain hydrogen bonds within the polymer network, thereby promoting stronger interactions between polymer chains and water molecules. However, as the salt concentration continues to increase, these beneficial interactions diminish due to excessive disruption of hydrogen bonding, resulting in salt precipitation. Thus, optimizing the salt concentration is crucial for preparing hydrogel electrolytes with optimal performance. For instance, Wei et al. developed a high-performance, processable crystalline gel electrolyte by using the dissolution–crystallization transition of sodium acetate (NaAc) in the hydrogel. The addition of NaAc crystals increases operating voltage (2.0 V) and the modulus (474.24 MPa) compared to the hydrogel without crystals. The resulting supercapacitors perform reliably in extremely low-temperature environments due to its phase-transition ability. Even at −40 °C, the specific capacitance can be maintained at 73.7% of the value at 20 °C (Fig. 11).57
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Fig. 11 Inorganic salt-modified hydrogel electrolytes enabling low-temperature operation of the supercapacitor. (a) In situ crystallization within a hydrogel matrix for the synthesis of crystalline composite gels. (b) Mechanical modulus and ionic conductivity of various non-liquid electrolytes. (c) Specific capacitance of gel electrolyte-based supercapacitors at various temperatures from −40 °C to 80 °C. Reproduced with permission.57 Copyright 2019, Wiley-VCH. |
Compared to traditional hydrogels, ionic liquid gels exhibit superior conductivity at low temperatures and improved thermal stability. Poly(ionic liquid) (PIL) hydrogels, synthesized from ionic liquid monomers, integrate the unique properties of ionic liquids with the structural advantages of polymer scaffolds. This enables PIL hydrogels not only to retain the physical/chemical characteristics of ionic liquids but also to benefit from the mechanical strength of polymers. For example, He et al. developed an innovative anti-freezing electrolyte based on a PIL hydrogel, which demonstrates high conductivity for energy storage applications. The anti-freezing gel electrolyte shows an impressive conductivity of 26 mS cm−1, while the assembled supercapacitors exhibit outstanding electrochemical performance, with a specific capacitance of 204 mF cm−2 at 1 mA cm−2. Notably, the supercapacitors retain 79.9% of their capacitance even at −20 °C, highlighting their remarkable low-temperature stability (Fig. 12).50
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Fig. 12 Anti-freezing PIL hydrogel electrolytes enabled by engineering hydrogen-bond networks. (a) Schematic diagram of the synthesis process of the PIL hydrogel. (b) Temperature-dependent ionic conductivity of the PIL hydrogel. (c) GCD profiles of PIL hydrogel-based supercapacitors at various temperatures with a current density of 1 mA cm−2. Reproduced with permission.50 Copyright 2023, Elsevier. |
Recently, theoretical simulations have become essential tools in low-temperature electrolyte research.72 Density functional theory (DFT), molecular dynamics (MD) and machine learning (ML) methods offer a deeper understanding of atomic or molecular-level interactions, providing valuable information such as ion coordination numbers, binding energies, electrostatic potentials, and the entropy of electrolytes.73,74 These methods provide valuable insights into electrolyte behavior at extremely low-temperatures that are otherwise difficult to access, such as electronic structure effects, solvation structure, and ionic diffusion mechanisms. The target temperature of multiscale models for electrolyte systems can be easily adjusted by modifying the code. To be more precise, DFT calculations can be utilized to elucidate the electronic-level interactions among electrolyte components, enabling a quantitative understanding of solvent–solvent, ion–solvent, and cation–anion interactions. Such first-principles approaches provide insights into binding energies, charge distributions, and interaction strengths at the atomic scale.47 Besides, MD simulations are typically employed to capture the time-resolved, statistical behavior of ions and solvent molecules, offering detailed information on solvation structures, dynamic rearrangements, and ion transport mechanisms under various conditions.75 Moreover, ML methods are being increasingly employed to expedite the screening of advanced low-temperature electrolytes, thereby circumventing the time- and resource-intensive trial-and-error approach. ML enables systematic analysis of experimental and theoretical data to establish electrolyte structure–property relationships, facilitating efficient identification of promising candidates. As validated through high-throughput experimentation, these findings can be incorporated into databases to further refine ML models. This approach not only accelerates the discovery of high-performance low-temperature electrolytes but also enables accurate prediction of electrochemical properties, demonstrating significant potential for advancing low-temperature energy storage systems.76 Such theoretical methods provide valuable insights into charging mechanisms when combined with advanced characterization techniques.77–79
As for advanced characterization techniques, IR spectroscopy plays a key role in the study of low-temperature electrolytes by providing valuable information about molecular vibrations and interactions.80 For the analysis of samples at low temperatures, special sample holders (such as liquid nitrogen-cooled sample cells) are typically used to keep the samples stable at such extreme temperatures. In general, IR spectroscopy serves as a useful tool for analyzing the solvation structure, offering valuable insights into the interactions between the solvent, additives, and ions in the electrolyte. For instance, Jiang et al. used IR spectroscopy to study the solvation structure of the electrolyte. With the addition of fluoroethylene carbonate (FEC)/ethyl acetate (EA), the alkyl C–H peak was found to be blue-shifted, suggesting an altered environment surrounding the C–H group on the imidazolium cation within the EMIMBF4-FEC/EA electrolyte compared to pure EMIMBF4. Furthermore, the addition of EA and FEC induced noticeable shifts of 2 and 3 cm−1 in the vibrational frequencies v(C2–H) and v(C4,5–H) of the imidazolium ring. Such significant shifts imply enhanced hydrogen bonding at these positions, which promotes a more uniform dispersion of the ionic liquids. This effect contributes to the decreased viscosity and enhanced ionic conductivity of the EMIMBF4-1F1E electrolyte over a broad temperature range (Fig. 13a).81 Moreover, the interactions can be notably altered at low temperatures due to changes in molecular motion and the formation of ion–solvent complexes. IR tests at low temperatures allow for the study of how the vibrational modes of electrolyte components change with temperature. Additionally, low temperatures may induce crystallization or phase transitions in certain electrolyte components, and such structural transformations can also be detected and characterized by IR spectroscopy. In short, IR spectroscopy can help researchers gain a deeper understanding of electrolyte properties and design advanced electrolytes for supercapacitors.
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Fig. 13 Overview of advanced characterization techniques for low-temperature electrolytes: (a) IR spectroscopy, reproduced with permission.81 Copyright 2024, Elsevier. (b) Raman spectroscopy, reproduced with permission.47 Copyright 2022, Royal Society of Chemistry. (c) NMR spectroscopy, reproduced with permission.87 Copyright 2024, American Chemical Society. (d) SAXS analysis, reproduced with permission.79 Copyright 2017, Springer Nature. (e) DLS measurements, reproduced with permission.90 Copyright 2023, Wiley-VCH. and (f) Cryo-EM imaging, reproduced with permission.61 Copyright 2022, Royal Society of Chemistry. |
Complementary to IR spectroscopy, Raman spectroscopy is a powerful technique that offers insights into molecular vibrations, bond interactions, and the local environment of ions and solvents, making it especially useful for studying electrolyte.82 Raman spectroscopy can identify specific functional groups in electrolyte components (such as solvents, ions, and additives) and monitor shifts in Raman peaks to detect changes in the chemical environment as temperature decreases. This helps track slight structural changes that affect electrolyte performance at low temperatures. For instance, Raman spectroscopy was employed to investigate the structural modulation of ionic liquid-based electrolytes induced by organic co-solvents. The characteristic S–N–S bending vibration of the TFSI− anion, observed at 740–750 cm−1, exhibited a red shift from 741.9 cm−1 to 738.5 cm−1 in the P-AN and P-AN-PC systems (P: [ionic liquid], AN: ACN, PC: methyl butyrate), indicative of hydrogen bonding between TFSI− and co-solvents. In contrast, no spectral shift occurred in the presence of ACN and methyl butyrate (MB), suggesting preferential hydrogen-bond interactions of these solvents with the ionic liquid's cation rather than the TFSI− anion. This coordination likely weakens the cation–anion interaction, facilitating the improved dispersion of ionic liquid. Furthermore, these interactions can account for the significant reduction in viscosity and the enhanced conductivity observed in the P-AN-MB system at low temperatures (Fig. 13b).47
NMR spectroscopy can provide detailed information about the local environment of solvents, ions, and their interactions with the electrolyte.78,83–86 In particular, NMR can be utilized to probe the interactions between different components of the electrolyte. By analyzing changes in chemical shifts and relaxation times, NMR provides insights into the local structural changes of the electrolyte, helping to identify the most suitable electrolyte formulations for supercapacitors. Representatively, NMR spectroscopy was employed to investigate the absorption behavior of an aqueous lithium bis(trifluoromethanesulfonyl)imide (LiTFSI) electrolyte by commercial activated carbon. The NMR results show rapid ion exchange between the bulk electrolyte and the ions within the carbon pores. These fast exchange processes significantly influence the apparent concentration of adsorbed Li+ and TFSI− ions, as quantified by NMR. The experiment suggests that as the electrolyte becomes more acidic, the carbon pores exhibit increased ionophilicity, which has crucial effects on the charge storage mechanisms in electrochemical systems (Fig. 13c).87 NMR instruments equipped with cryoprobes can perform the tests at low temperatures, revealing how ions are solvated in different electrolyte composition at low temperatures, which is critical for optimizing low-temperature performance of supercapacitors. Examining changes in the NMR spectra at various temperatures is important for understanding how the charge storage capability is affected by temperature.
Small-angle X-ray scattering (SAXS) can provide valuable insights into the ion adsorption behaviors in nano and sub-nano channels.71,88,89 As a typical example, Prehal et al. elucidated voltage-dependent ion redistribution in aqueous electrolytes confined within three microporous carbons using in situ SAXS. By coupling experimental SAXS data with theoretical simulations, their methodology reveals the correlations between electric-field-driven ion confinement/desolvation and capacitive behavior, advancing the rational design of carbon-based energy storage systems (Fig. 13d).79 In general, electrolyte ions may exhibit different behaviors at low temperatures, such as increased ion pairing or aggregation due to lower thermal motion. SAXS can detect changes in the scattering pattern that correspond to these structural changes. By analyzing the scattering profile, researchers can gain insights into the solvation structure and how they are influenced by temperature or electrolyte composition.
Dynamic light scattering (DLS) is a versatile technique commonly used to analyze particle size distribution and dynamics in colloidal suspensions, making it particularly useful for studying the behavior of electrolytes at low temperatures.90 DLS can be used to monitor temperature-dependent changes in the size of ion clusters, aggregates, or nanoparticles in low-temperature electrolytes. In liquid electrolytes, particularly ionic liquids or gel-based systems, ions may aggregate or form clusters at lower temperatures, potentially affecting conductivity and electrochemical performance. DLS allows for the detection and quantification of such aggregation, providing insights into its impact on ionic transport. If aggregation results in larger clusters or phase separation, DLS can help inform adjustments to electrolyte composition to minimize negative effects on supercapacitor performance. For instance, Shi et al. employed DLS measurements to unravel micelle self-assembly behavior in a 1 M LiFSI electrolyte, revealing particles with an average diameter of approximately 3.14 nm. The observed Tyndall effect further supports these findings. Both simulation and experimental data confirm that the introduction of the amphiphilic 1,1,2,2-tetrafluoro-3-methoxypropane (TFMP) cosolvent facilitates the self-assembly of the electrolyte, leading to the formation of a core-shell-like solvation structure. This distinctive solvation structure enhances ion conductivity and enables facile desolvation, demonstrating superior cyclability at low temperatures (Fig. 13e).90
Cryogenic electron microscopy (Cryo-EM) is a cutting-edge imaging technique primarily used for the detailed study of biological macromolecules at high resolution, but it has also found applications in the study of electrolytes.91–94 Cryo-EM provides significant advantages in examining the structural and morphological properties of electrolytes at near-freezing temperatures. At low temperatures, electrolytes may undergo phase transitions like crystallization, gel formation, or aggregation, which can hinder ion mobility and decrease conductivity. Cryo-EM allows for high-resolution imaging of these processes, offering valuable insights into electrolyte behavior under low-temperature conditions and their impact on supercapacitors performance. Real-time imaging can identify these transitions, aiding the development of more stable electrolytes for supercapacitors in cold environments. For example, Tu et al. used cryo-SEM and cryo-TEM to examine the morphological characteristics of the ion-conducting gel (IG). SEM observations of the IG membrane exhibit a smooth, homogeneous surface without visible crystalline CuSO4 aggregates, suggesting favorable compatibility between the PVA matrix and the CuSO4 species. Furthermore, cryo-TEM analysis was conducted to explore the internal structure of the IGs. The resulting images revealed an amorphous morphology within the bulk phase, with no distinct signs of CuSO4 crystallization. These findings imply that the PVA solution underwent freezing into a glassy, non-crystalline state, in which Cu2+ and SO42− ions were uniformly dispersed. The uniform distribution of molecules/ions will facilitate the formation of ion channels, ensuring efficient ion migration within the IGs (Fig. 13f).61
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Fig. 14 Overview and future perspectives on the development of low-temperature electrolytes for high-performance supercapacitors. |
(1) Optimizing the multiple physical parameters of electrolytes to achieve optimal overall performance and establishing standardized evaluation criteria: recent studies have predominantly focused on pursuing extremely low operational temperatures, with excessive emphasis placed on depressing the freezing point of electrolytes. However, other critical performance parameters of electrolytes are often neglected, including viscosity, ionic conductivity, and electrochemical stability window. Such unilateral optimization approaches may compromise the overall electrochemical performance under low-temperature conditions. Therefore, a more comprehensive set of evaluation criteria for low-temperature electrochemical performance should be established to enable a more objective and holistic assessment of device behavior at low temperatures. Future research should embrace a holistic design paradigm that concurrently optimizes multiple physicochemical parameters alongside the development of low-melting-point electrolytes, thereby enabling a comprehensive enhancement in low-temperature electrochemical performance.
(2) Developing novel strategies to construct high-performance electrolyte systems: beyond conventional approaches such as salt selection or solvent optimization, future research should explore unconventional electrolyte architectures. For instance, integrating entropy-driven design principles, weak solvation strategies, deep eutectic solvents, and advanced additive engineering can enable the simultaneous optimization of multiple critical parameters of electrolytes and improve low-temperature performance. In the future, collaborative efforts spanning materials, chemistry, and physics science are anticipated to unveil novel anti-freezing mechanisms and foster innovative breakthroughs in the design of next-generation electrolyte systems, thereby achieving robust electrochemical performance under extreme temperature conditions.
(3) Investigating and establishing the connection between the microstructure and the low-temperature performance of electrolyte: for instance, the solvation structure and desolvation process play a critical role in governing ion transport at the solid–liquid interface. At low temperatures, sluggish ion mobility and hindered interfacial charge transfer often arise from rigid solvation shells and limited desolvation kinetics. A detailed understanding of how the electrolyte's local coordination environment, ion pairing behavior, and solvent dynamics evolve under low-temperature conditions can provide critical insights into the ion transport limitations. Moving forward, tailoring solvation structures through molecular design, such as the incorporation of asymmetric solvents, weakly coordinating solvents, or fluorinated species, holds great promise in promoting efficient desolvation and enhancing ion transport kinetics. Ultimately, such microstructure-performance insights will lay a solid foundation for the rational design of next-generation electrolytes specifically engineered for high-performance supercapacitors in low-temperature environments.
(4) Developing advanced computational methods to screen effective electrolyte components and predict their low-temperature performance: although DFT calculations and MD methods can shed new light on the microscopic structure of electrolytes, the rise of ML technology will provide more intelligent solutions for the design of low-temperature electrolytes. By training predictive models on high-quality experimental and simulation datasets, ML methods can rapidly identify correlations between molecular structure, solvation characteristics, and low-temperature electrochemical performance. Furthermore, ML methods offer powerful capabilities in identifying latent patterns and complex nonlinear relationships that often elude conventional analytical approaches. The advancement of ML methods can effectively reduce the cost of trial-and-error processes and improve efficiency. In the long term, the construction of comprehensive electrolyte databases and the adoption of active learning and generative models may enable the inverse design of low-temperature electrolytes with desired physicochemical properties.
(5) Developing advanced in situ characterization techniques to unveil energy storage mechanisms at low temperature: currently, many existing characterization techniques lack low-temperature operability. This presents a significant bottleneck in the mechanistic understanding of low-temperature electrochemical phenomena. Developing novel cell designs or equipment that can adapt current characterization tools to low-temperature environments could provide new insights into this area. For instance, innovative efforts are needed to engineer bespoke electrochemical cells and integrated setups capable of maintaining precise temperature control while ensuring compatibility with a wide range of spectroscopic and microscopic techniques. The development of cryo-compatible in situ cells, vacuum-insulated chambers, or microfluidic platforms with localized temperature regulation could enable real-time monitoring of solvation dynamics, ion transport behavior, and electrode–electrolyte interface evolution under realistic working conditions. By enabling direct observation of the structural, chemical, and electrochemical changes that occur in low-temperature environments, these advanced characterization strategies will provide critical insights for the rational design of low-temperature electrolyte systems for supercapacitors.
(6) Enhancing low-temperature performance by optimizing supercapacitor components beyond the electrolyte: in addition to the electrolyte, the construction of advanced electrode materials tailored for low-temperature electrolytes is of paramount importance. While existing studies predominantly emphasize lowering the freezing point and improving the ionic conductivity of low-temperature electrolyte, insufficient attention has been paid to the design and optimization of electrode materials that are well-matched with such electrolytes. Given their pivotal role in supercapacitors, the microstructure, specific surface area, pore architecture, and electrical conductivity of electrode materials critically affect device performance. Thus, it is imperative to advance electrode materials that are compatible and synergistic with the electrolyte systems. Moreover, other components such as current collectors, separators, conductive additives, and binders also exert significant influence on the electrochemical performance at low temperatures. Therefore, it is essential to rationally optimize and integrate these components to achieve optimal electrochemical performance of supercapacitors at low temperatures.
Overall, despite significant advancements in low-temperature supercapacitors in recent years, the design of efficient electrolytes suitable for low-temperature applications remains a critical challenge. Considering the rising demand for energy storage systems capable of reliable operation in cold environments, the prospects for advanced low-temperature electrolytes are highly promising. With intensified research efforts in this field, novel computational approaches and advanced characterization techniques are being continuously developed to elucidate the microstructure of electrolytes and investigate their energy storage mechanisms. We anticipate continuous breakthroughs that will ultimately accelerate the commercialization and widespread applications of low-temperature supercapacitors.
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