Ionic Liquid-Based Electrolytes for Energy Storage Devices: A Brief Review on Their Limits and Applications

Since the ability of ionic liquid (IL) was demonstrated to act as a solvent or an electrolyte, IL-based electrolytes have been widely used as a potential candidate for renewable energy storage devices, like lithium ion batteries (LIBs) and supercapacitors (SCs). In this review, we aimed to present the state-of-the-art of IL-based electrolytes electrochemical, cycling, and physicochemical properties, which are crucial for LIBs and SCs. ILs can also be regarded as designer solvents to replace the more flammable organic carbonates and improve the green credentials and performance of energy storage devices, especially LIBs and SCs. This review affords an outline of the progress of ILs in energy-related applications and provides essential ideas on the emerging challenges and openings that may motivate the scientific communities to move towards IL-based energy devices. Finally, the challenges in design of the new type of ILs structures for energy and environmental applications are also highlighted.


Introduction
In the recent times, most of the transportable smart devices and some of the hybrid electric vehicles, which are marketed to present day customers, are equipped with the light weight electrochemical energy storage (EES) devices, include lithium-ion batteries [1][2][3][4] (LIBs) and supercapacitors [5][6][7][8] (SCs), which is the backbone of commercially available portable electronic devices [9,10]. However, to date, uses of LIBs and SCs as a power sources for large scale applications, including electric vehicles, are a distant reality. Operational safety is one of the vital reasons hindering their use for large scale application; hence, their widespread uses need to be addressed. In addition, the transport property hindering their use for large scale application; hence, their widespread uses need to be addressed. In addition, the transport property and structural stability of the ionic species are extremely crucial and responsible for the efficient outputs in energy storage devices. In the light of this fact, high current (i.e., automotive applications) operating devices are required to have storage devices that have higher power density and faster ion transport properties. Previous studies have suggested that one of the most favorable approaches to simultaneously progress the safety, along with energy and power densities, is the incorporation of ILs into the electrolyte system [11].
In past decades, room temperature ionic liquids (RTILs) have been acknowledged with noteworthy attention due to their excellent miscellaneous properties, such as thermal and chemical stability, tunable structure over the wide range of operating temperature, a broad electrochemical stability window, high ionic conductivity in the range of 10 −3 -10 −2 S cm −1 at room temperature, and non-flammability as a potential candidate for EES devices, such as LIBs [12], electric double-layer SCs [13][14][15], proton exchange membrane fuel cells, and solar cells [16][17][18][19]. Using ILs as an alternative to organic electrolytes has the advantage of improving the ions' mobility, as well as eliminating the hazards associated within the organic electrolytes. Additionally, ILs often have comparable zero or negligible vapor pressure at normal temperatures due to their high thermal stability. Because of the above statements, ILs are widely used as solvents or electrolytes for energy storage applications in recent times [7,18,[20][21][22][23][24][25][26][27].
In this review, we aimed to present the recent developments of IL-based electrolytes for their potential applications in LIBs and SCs. Additionally, some of the strategies, opportunities, and challenges are discussed for the more rational design of ILs structures to make it more suitable for fabricating green EES devices. Especially, discussions are focused to cover-up the outstanding physicochemical and electrochemical properties of some potentially modified electrolytes with ILs for their applications in energy storage systems. However, to keep this review short, precise, and useful to present-day researchers, this review assessed, examined, and discussed articles published after 2010; therefore, some of the excellent research works prior to 2010 are not cited. To avoid plausible distractions, the content of this review article is divided into two different broad categories, as follows: (a) IL-based electrolytes for LIB applications and (b) IL-based electrolytes for SC applications. A schematic representation of IL-based electrolytes employed in LIBs and SCs is denoted in Figure 1.

IL-Based Electrolytes for LIBs Application
It is well known that the specific energy densities of LIBs are quite high compared to other conventional batteries and SCs, but it certainly needs improvement in terms of power density. To improve LIBs power density, LIBs components, such as anode, cathode, and electrolytes, are deeply investigated and various replacements have been reported elsewhere [48,49]. To date, various electrolytes have been prepared and employed in this aspect. Moreover, this part of review is focused on the IL-based liquid, gel, and solid polymer electrolytes prepared by various techniques/activation processes for LIB applications.
In general, the LIB mainly consists of three components: (1) the positive electrode, which is typically based on metal oxides and phosphates; (2) the negative electrode, which is generally graphite or metallic lithium; and (3) an electrolyte, which can be either in a solid, liquid, or gel form. Electrolytes facilitate the migration of ionic charge carriers within the LIBs and are hence considered to be the heart of LIBs [50,51]. To be a good electrolyte, certain characteristics in nature are necessary in the electrolyte comprised LIBs for stable and safe operation. The important functions of electrolytes in LIBs are as follows: (a) the rapid migration properties during the charge-discharge process between the two electrodes, which is essential to transport of lithium ions; (b) robustness of electrochemical and chemical properties; (c) the high boiling point and low melting point, which are crucial for broad region of operating temperatures; (d) negligible vapor pressure at room temperature, which reduces the flammability of the electrolyte. Although different types of electrolytes have been designed and employed in LIBs, the two most widely accepted are liquid and polymer electrolytes (which can be further categorized into solid, gel, and composite electrolytes).

Organic Carbonates and Ionic Liquid-Based Binary Liquid Electrolytes
In general, during battery operations, the electrolytes of organic solvents which have inflammable properties may imitate the fire or explosions owing to the abominable conditions or short circuit. Thus, operational safety issues must be addressed before it could be widely launched for practical applications. To advance operational safety, ILs have been incorporated with an organic carbonate-based electrolyte that has efficiently enhanced the thermal stability of lithium cells [52]. In addition, IL has better conductivity compared to conventional organic electrolytes, and it could be overwhelmed by the inclusion of selective carbonates in the ILs, ensuing the development of low viscous mixtures and thereby further improving the conductivity and thermal stability [53]. From this perspective, ILs have been broadly considered and are regarded as one of the secured electrolytes for LIB applications because of their excellent properties, such as high ionic conductivity, negligible vapor pressure, low flammability, and high thermal stability. In addition, maximum ILs have better ionic conductivity and considerable electrochemical stability; hence, they are outstanding alternatives to flammable organic carbonate solvents. Furthermore, the choice of the anions and cations in ILs is very important, and it plays a vital role in evaluating the viscosity and solubility of ILs [37,43].
Among the different families of ILs, the ILs containing TFSI anions and PYR cations have been widely studied and used for LIB applications, owing to their excellent electrochemical and thermal stabilities [33,42,54,55]. Between the TFSI anionic ILs, 1-butyl-3-methylpyrrolidinium bis(trifluoromethanesulfonyl)imide (PYR 14 TFSI) is of particular interest because of its excellent air and thermal stabilities (up to 300 • C). It also exhibits a cathodic stability more than 5.5 V, which makes it a potential electrolyte candidate for LIBs [52,56]. Kuhnel et al. prepared and investigated a ternary electrolyte mixture that contains PYR 14 TFSI and lithium bis(trifluoromethanesulfonyl)imide (LiTFSI), along with a propylene carbonate (PC) solvent [52]. Interestingly, it was observed that the properties can be tuned by adjusting the amount of IL in electrolyte mixtures. It was found that the mixture containing 80 wt% IL has non-flammable properties, with promising cycling performance, at room temperature and 60 • C, as well [52]. Likewise, the flammability and thermal stability of the electrolyte solutions of 1-butyl-1-methyl pyrrolidinium bis(trifluoromethanesulfonyl)imide (PYR 14  were thoroughly investigated by Ye et al. [57]. They used the carbonate solvents as solid electrolyte interphase (SEI)-forming additives that can make a firm SEI layer over the electrode and protect the electrode from the reductive decomposition of the IL. From their experiments, they observed that the inflammability and capacity declining of the electrolytes were found to be enormously decreased due to the addition of VC along with the IL. Hofmann et al. [58] investigated the behaviors of poly(vinylidene fluoride) hexafluoropropylene (PVdF-co-HFP) polymer electrolytes based on ILs (PYR 13 ), lithium bis(trifluoromethylsulfonyl)azanide, and organic carbonates as electrolyte components. Interestingly, the maximum discharge capacity achieved at 100 mA h g −1 for a graphite/IL-EC/PC electrolyte/lithium manganese nickel cobalt oxide (LiMNC) cell [58]. In addition, ILs, such as PYR 14 TFSI, 1-methoxyethoxymethyl(tri-n-butyl)phosphonium bis(trifluoromethanesulfonyl)amide (MEMBu 3 PTFSI), N-propyl-n-methylphosphonium bis((trifluoromethanesulfonyl imide (PP 13 TFSI), and organic carbonates electrolytes, has demonstrated strong combined effect which caused the high reversibility of lithium ion intercalation, as well as reduction of SEI formation over the electrode-electrolyte interfaces [2,59].
The inclusion of ILs in organic carbonates have reduced the electrochemical stability window profoundly compared to pure ILs, which is proved in the lot of related literatures [36,[60][61][62][63]. In the meantime, the compatibility between the electrolyte and electrode leads to improve the anodic stability greatly. For instance, the electrolyte 0.5 M lithium nitrate (LiNO 3 ) in PC-pyrrolidinium nitrate (PYRNO 3 ) exhibited good conductivity and an electrochemical stability window that is great enough to assure the safe de-insertion and insertion of lithium into LiFePO 4 [64][65][66][67]. A new type of organic liquid electrolyte, consisting of Pip 13 TFSI and dimethoxyethane (DME), was studied and reported their improved cell specific capacity and cycle life in lithium-metal batteries [68][69][70]. The comparison diagram of conducting properties of different types of electrolytes used for LIBs [71][72][73][74][75] is shown in Figure 2. In the conductivity plot of LIBs, the conductivity of pristine ILs are three orders better than conventional organic liquid electrolyte and gel polymer electrolytes, which is due to better ions-mobility of ILs. Further, it acts as a co-solvent during the preparation of electrolytes that avoid the solvent effect in electrolyte films.  [57]. They used the carbonate solvents as solid electrolyte interphase (SEI)-forming additives that can make a firm SEI layer over the electrode and protect the electrode from the reductive decomposition of the IL. From their experiments, they observed that the inflammability and capacity declining of the electrolytes were found to be enormously decreased due to the addition of VC along with the IL. Hofmann et al. [58] investigated the behaviors of poly(vinylidene fluoride) hexafluoropropylene (PVdF-co-HFP) polymer electrolytes based on ILs (PYR13), lithium bis(trifluoromethylsulfonyl)azanide, and organic carbonates as electrolyte components. Interestingly, the maximum discharge capacity achieved at 100 mA h g −1 for a graphite/IL-EC/PC electrolyte/lithium manganese nickel cobalt oxide (LiMNC) cell [58]. In addition, ILs, such as PYR14TFSI, 1-methoxyethoxymethyl(tri-n-butyl)phosphonium bis(trifluoromethanesulfonyl)amide (MEMBu3PTFSI), N-propyl-n-methylphosphonium bis((trifluoromethanesulfonyl imide (PP13TFSI), and organic carbonates electrolytes, has demonstrated strong combined effect which caused the high reversibility of lithium ion intercalation, as well as reduction of SEI formation over the electrode-electrolyte interfaces [2,59].
The inclusion of ILs in organic carbonates have reduced the electrochemical stability window profoundly compared to pure ILs, which is proved in the lot of related literatures [36,[60][61][62][63]. In the meantime, the compatibility between the electrolyte and electrode leads to improve the anodic stability greatly. For instance, the electrolyte 0.5 M lithium nitrate (LiNO3) in PC-pyrrolidinium nitrate (PYRNO3) exhibited good conductivity and an electrochemical stability window that is great enough to assure the safe de-insertion and insertion of lithium into LiFePO4 [64][65][66][67]. A new type of organic liquid electrolyte, consisting of Pip13TFSI and dimethoxyethane (DME), was studied and reported their improved cell specific capacity and cycle life in lithium-metal batteries [68][69][70]. The comparison diagram of conducting properties of different types of electrolytes used for LIBs [71][72][73][74][75] is shown in Figure 2. In the conductivity plot of LIBs, the conductivity of pristine ILs are three orders better than conventional organic liquid electrolyte and gel polymer electrolytes, which is due to better ions-mobility of ILs. Further, it acts as a co-solvent during the preparation of electrolytes that avoid the solvent effect in electrolyte films.  Depending on the ionic structure, ILs can be either protic or aprotic. Due to enormous available cations and anions structure, different combinations of ILs were studied. Figure 3 shows the cations Polymers 2020, 12, 918 5 of 37 and anions structure of some important ILs for energy storage systems that are discussed in this review. As we know, the bigger the size of the anion, the weaker the coordination between cation and anion, which in turn facilitates the dissociation of ions very easily in the solvent medium. Recent reports have revealed that the IL electrolytes with bis(fluorosulfonyl imide) (FSI) anions (FSI − ) exhibit higher ionic conductivities and lower viscosities, which are due to the lesser dimensional size of the FSI − compared to the TFSI anion [42,73]. In some circumstances, the ILs, together with a carbonate solvent, showed a higher viscosity and lower conductivity, which resulted in poor cycling behaviors than that of the organic electrolytes (LiPF 6 in organic carbonates), particularly at high-rate cycling performances. This is due to the following factors: (i) the formation of an inaccurate random SEI layer on the negative electrodes [76] and (ii) sluggish migration of ions and cumbersome absorption of porous electrodes [77]. Depending on the ionic structure, ILs can be either protic or aprotic. Due to enormous available cations and anions structure, different combinations of ILs were studied. Figure 3 shows the cations and anions structure of some important ILs for energy storage systems that are discussed in this review. As we know, the bigger the size of the anion, the weaker the coordination between cation and anion, which in turn facilitates the dissociation of ions very easily in the solvent medium. Recent reports have revealed that the IL electrolytes with bis(fluorosulfonyl imide) (FSI) anions (FSI − ) exhibit higher ionic conductivities and lower viscosities, which are due to the lesser dimensional size of the FSI − compared to the TFSI anion [42,73]. In some circumstances, the ILs, together with a carbonate solvent, showed a higher viscosity and lower conductivity, which resulted in poor cycling behaviors than that of the organic electrolytes (LiPF6 in organic carbonates), particularly at high-rate cycling performances. This is due to the following factors: (i) the formation of an inaccurate random SEI layer on the negative electrodes [76] and (ii) sluggish migration of ions and cumbersome absorption of porous electrodes [77]. Liao et al. [76] reported the prime application of sulfolane (SL), mixtures of SL with the conducting salt LiClO4 and carbonates (DMC, PC) in LIB cells. Yet, an ultra-quick capacity fading was detected in graphite anode compartment. Li et al. evidenced the feasibility of sulfites and SL blend as electrolyte solvents with conducting salt of lithium bis(oxalato) borate (LiBOB), which results in the reduction of the flashpoints significantly for practical application of LIBs [78]. To overcome the aforesaid issues, most research has focused on identifying new ILs with negligible vapor pressures and high flash points for LIBs [54,[79][80][81][82].
Recently, 1-allyl-3-methylimidazolium (AMIm)TFSI and 1-methyl-3-propylimidazolium (Im13)TFSI-based electrolytes with PC were compared by Wang et al. and revealed the formation of (in an 1-allyl-3-methylimidazolium bis(trifluoromethanesulfonyl)imide (AMImTFSI)-based electrolyte) a firm protective layer over the electrode surface, which supports subduing the decomposition of solvent and increasing the cycling behavior of the LIBs [83]. They reported that the Li/LiFePO4 coin cell delivered the stable discharge capacities of ~151 mA h g −1 after 100 cycles at 0.1 C rate, with a retention of 97.4%. Similar behavior was exhibited for PYR14TFSI, as well as Liao et al. [76] reported the prime application of sulfolane (SL), mixtures of SL with the conducting salt LiClO 4 and carbonates (DMC, PC) in LIB cells. Yet, an ultra-quick capacity fading was detected in graphite anode compartment. Li et al. evidenced the feasibility of sulfites and SL blend as electrolyte solvents with conducting salt of lithium bis(oxalato) borate (LiBOB), which results in the reduction of the flashpoints significantly for practical application of LIBs [78]. To overcome the aforesaid issues, most research has focused on identifying new ILs with negligible vapor pressures and high flash points for LIBs [54,[79][80][81][82].
They employed three-dimensional nano-silicon electrodes as a working electrode with the metallic lithium as a reference cum counter electrode. It exhibited the highest specific capacities of 1912 mA h g −1 and 2230 mA h g −1 at 0.41 and 0.52 mA h cm −2 , respectively. Xia Cao et al. revealed extraordinary progress with regard to capacity retention and columbic efficiency at elevated temperatures for LNMO/Li 4 Ti 5 O 12 (LTO) cells containing LiTFSI/PYRTFSI electrolytes [89].

Pristine Ionic Liquids as Electrolytes
As we discussed earlier, the commercially available liquid electrolytes that consist of mixed organic solvents (linear and cyclic carbonates) and LiPF 6 are highly flammable and thermally unstable Polymers 2020, 12, 918 7 of 37 at high temperatures [12,27,87,90]. To attain a maximum level of safety for LIBs, the progress of thermally stable electrolytes is the decisive one. For this, RTILs have been paid great consideration in the past due to their exceptional properties in terms of electrochemical and thermal stabilities [77,91]. Hence, in order to develop the solvent-free electrolytes, the RTILs, also known as "designer solvents", have tunable properties, which is a valid alternative to replace carbonate solvents [21]. This section will thoroughly discuss the utilization of RTILs as "solvents" for dissolving lithium salts and acting as a pure electrolyte for LIB applications.
In the past decade, imidazolium and PYR-based ILs have become promising potential candidate for LIBs applications. These two IL families' have a better ionic conductivity and low viscosity compared to other ILs and can allow the electrochemical intercalation as lithium into cathode materials, important industrial requirements for practical purposes. Some of the important niceties of these two families of ILs are discussed as follows: Archer et al. extensively studied silica nanoparticle-tethered Im 13 TFSI from the applied and fundamental perspectives. They revealed that the inclusion of nanoparticles in the electrolyte system hindered the crystallization of lithium salt (by means of the interactions between the TFSI counter-ion salt and the tethered cations of the IL surface), thereby enhancing lithium ion mobility, transference numbers, and the mechanical properties of the electrolytes [92,93].
Likewise, its analogous 1-ethyl-3-methylimidazolium bis(fluorosulfonyl)amide Im 13 FSI IL interaction with LiTFSI was elaborately and extensively analyzed through Raman spectroscopy by Fuji et al. [94,95]. They found that the lithium-ion solvation in FSI anion-based ILs is rather different from TFSI ion-based ILs, even though both anions have similar molecular structures and environments. Interestingly, the same anion interactions with PYR-based cations were experimentally and theoretically investigated by several groups [96][97][98].
Later, Deshpande et al. studied the flexibility and migration characteristics of lithium ions in PYR 13 TFSI ILs and characterized the electrolyte system using the molecular dynamics method [99]. These detected molecular dynamics and electrochemical (electrolyte ions mobility) results are in great agreement with the previous literatures using PYR as a cationic IL [100,101].
Based on the interactions between ILs and lithium salts as discussed above, several research groups have tried to enhance the other properties, such as the thermal, electrochemical, and cycling stabilities, for these kinds of liquid electrolytes [46,[101][102][103][104][105][106]. The 1 M LiTFSI in PYR 14 TFSI electrolyte has showed better electrochemical and cycling properties with commercial liquid electrolytes [77] (1 M LiPF 6 in EC/DEC).

Ionic Liquid-Based Gel Polymer Electrolytes
Commercial LIBs are comprised of LiPF 6 in a mixture of carbonate solvents as the electrolyte [57,115,116]. When the cell operates, the anion present in lithium salt undergoes an equilibrium reaction and forms a Lewis acid PF 5 . This Lewis acid, in turn, reacts with the organic solvents EC/PC. The P-F bonds thus formed easily undergo hydrolysis, even if trace quantity of moisture is in the electrolyte medium, which, in turn, affects the performance of LIBs, hence making these solvents highly unsuitable [77,[117][118][119]. Hence, in order to overcome the abovementioned issues, better alternatives of hydrophobic IL electrolytes are found to be one of the most promising electrolytes for LIBs, providing the stability for lithium electrode from air or moisture due to its hydrophobic-nature.
Further, gel polymer electrolytes (GPEs) satisfy numerous requirements, like high ionic conductivity at ambient temperature, compatibility with the electrodes, a broad electrochemical window, no leakage, better thermal and appropriate mechanical stabilities, etc., for their practical use in LIB cell. Furthermore, they possess two main advantages: firstly "solid-like" soft matter electrolytes with physicochemical properties superior to IL-based electrolytes without polymer host; and, secondly, lithium cell assembly also involves an only solid material, which is achieved by using the polymer as one of the medium.
The formation of a GPE using lithium ion conducting salt, IL, and PMMA polymer host is pictorially represented in Figure 4a [123]. The formation of PMMA-IL-TFSI-based electrolytes exactly follow the percolation threshold mechanism of polymers as reported earlier by Monalisa et al. [126]. It involved, at ambient temperatures, the concentration of amorphous regions well below the percolation threshold, which in turn lead to the lower value of ionic conductivity, as represented in the left-hand side of  Some of the recent literature strongly favors the utilization of ILs in GPEs to greatly enhance the conducting properties and cycling performance of the LIBs, which are summarized as follows. Patel et al. [127] investigated the room temperature IL gel polymer electrolyte LiTFSI-PYR14TFSI for application in LIBs using acrylonitrile monomer as the host. Interestingly, compared to pristine ILs, they observed better cycling performance and rate capability (current density 35-760 mAg −1 ) with LiFePO4 electronically wired with multi-walled carbon nanotubes (MWCNT) cathode, which indicates the polymer framework is capable of delivering excellent tracks for the rapid ions migration.
Likewise, a Pip13TFSI + LiTFSI/VC in a PVdF-co-HFP network exposed the maximum capacity of 340 mA h g −1 [128]. Rao et al. [124] prepared GPEs membrane based on electrospinning technique, which contained PAN/PMMA polymer host incorporated with an IL PYR14TFSI and delivered the supreme conductivity of 3.6× 10 −3 S cm −1 , and it was unwavering for the high potential of more than 5 V vs. Li + /Li. The capacities of Li/GPE/LiFePO4 cells were found to be 139, 134, 120, and 101 mA h g −1 at the rate of 0.1, 0.2, 0.5, and 1 C, respectively, which is higher than previously reported PAN electrospun GPE membranes [129,130].
Recently, Liao et al. [130] constructed a half-cell Li/GPE 80 wt% PYR13TFSI/LiFePO4 that showed a discharge capacity of 90 mA h g −1 at 0.1 C, mainly owing to the intrinsically low conductivity of membrane at ambient temperature. In addition, they observed the improved cell performance by cycling at 50 °C , but it typically resulted in a lower columbic efficiency due to the increased sensitive nature of the electrolyte with anode.
ILs are purely responsible for the ionic transport/migration properties, as well as the amorphicity of the gel membranes. For instance, Shalu et al. prepared and examined Some of the recent literature strongly favors the utilization of ILs in GPEs to greatly enhance the conducting properties and cycling performance of the LIBs, which are summarized as follows. Patel et al. [127] investigated the room temperature IL gel polymer electrolyte LiTFSI-PYR 14 TFSI for application in LIBs using acrylonitrile monomer as the host. Interestingly, compared to pristine ILs, they observed better cycling performance and rate capability (current density 35-760 mAg −1 ) with LiFePO 4 electronically wired with multi-walled carbon nanotubes (MWCNT) cathode, which indicates the polymer framework is capable of delivering excellent tracks for the rapid ions migration.
Likewise, a Pip 13 TFSI + LiTFSI/VC in a PVdF-co-HFP network exposed the maximum capacity of 340 mA h g −1 [128]. Rao et al. [124] prepared GPEs membrane based on electrospinning technique, which contained PAN/PMMA polymer host incorporated with an IL PYR 14 TFSI and delivered the supreme conductivity of 3.6 × 10 −3 S cm −1 , and it was unwavering for the high potential of more than 5 V vs. Li + /Li. The capacities of Li/GPE/LiFePO 4 cells were found to be 139, 134, 120, and 101 mA h g −1 at the rate of 0.1, 0.2, 0.5, and 1 C, respectively, which is higher than previously reported PAN electrospun GPE membranes [129,130].
Recently, Liao et al. [130] constructed a half-cell Li/GPE 80 wt% PYR 13 TFSI/LiFePO 4 that showed a discharge capacity of 90 mA h g −1 at 0.1 C, mainly owing to the intrinsically low conductivity of membrane at ambient temperature. In addition, they observed the improved cell performance by cycling at 50 • C, but it typically resulted in a lower columbic efficiency due to the increased sensitive nature of the electrolyte with anode.
ILs are purely responsible for the ionic transport/migration properties, as well as the amorphicity of the gel membranes. For instance, Shalu et al. prepared and examined PVdF-co-HFP-based ternary gel polymer electrolytes (TGPEs) using EMImBF 4 and LiBF 4 , and their ionic conductivity, as well as the amorphicity, was enhanced with an increase in the concentration of Im 13 BF 4 [40]. This may due to the decline of polymer crystallinity by the addition of Im 13 BF 4 [131,132]. Similar kinds of behavior have been observed for other TGPEs containing ILs, such as Pip 13 TFSI [12,128], PYR 1,4 TFSI [3,23,35], Pip 13 BETI [133,134], and Im 13 TFSI [134].
Recently, many research groups, including our group, have investigated the mechanism behind the transport properties of TGPEs using different types of ILs, which include Im 13 NfO [45], Im 14 NfO [44], Im 13 DFOB [135], Im 13 SCN [46] complexes with PVdF-co-HFP. In particular, Im 13 DFOB IL's addition in PVdF-co-HFP significantly enhanced the room temperature conductivity (10 −5 S cm −1 ), along with the stability window of 4.25 V. The transference number and cycling performance (148.4 mA h g −1 ) of the IL-GPEs increased drastically after EMImDFOB addition [135]. Pitwala et al. recently examined the consequence of various pyrrolidinium-based ILs, such as PYR 14 , PYR 24 , and TFSI, on the conducting and ion interaction properties of PVdF-co-HFP-based GPEs [34].
The GPEs have been further extended by way of incorporating Al 2 O 3 into the PMMA host, which are called quaternary polymer electrolytes (QPEs), drastically enhancing the thermal and cycling stabilities of the GPEs [91] by the way of crosslinking with the polymer host, which, in turn, to reduce the lithium ion (Li + ) transport distance, thereby creates more lithium-ion conducting pathways. A similar type of quaternary polymer electrolyte (QPE) investigated by Li et al. using 1g 13 TFSI IL, LiTFSI, SiO 2 , and PMMA precursors. These prepared QPEs possessed thermal solidity (300 • C), robust electrochemical property with broad stability window (4.0 V), rapid ion migration property, interfacial stability, and excellent charge/discharge behavior due to the addition of nanosilica and 1g 13 TFSI [136]. Moreover, the anodic stability of the QPEs was increased enormously with the incorporation of dimeric ILs in the polymer host matrix [137], and it might be attributed to the formation of passive layers over the anode surface, which creates the massive growth of cells. Dissimilarly, the massive growth was not formed for a dense structure with uniform deposition of lithium. Hence, for anodic stability enhancement, it is important to minimize the formation of passive layers over anode, which is schematically illustrated in Figure 5a [137]. From Figure 5a, it is observed that it consists of two important phase regions (a) polymer-enriched medium and (b) liquid enriched medium. Figure 5a represents the carbonate solvent-based gel electrolytes which enhance the lithium ion concentration and deposit over the surface of the metal anode in a non-uniform manner to form a porous structure. The introduction of IL PDMITFSI in gel matrix occupies the interface of polymer enriched medium and the liquid electrolyte-enriched medium as shown in Figure 5b which in turn reduced the domains size of dispersed liquid electrolyte and increases the number of electrolyte-rich phase. This behavior is likely to boost the Li + concentration in liquid electrolyte and thus lithium deposited uniformly in a particle-like a shape structure over the electrode surface and also regulate the dendrite free anode at the interface. A similar type of behaviors was observed by Park et al. [138] for PYR 1,4 TFSI IL electrolyte and few-layer graphene coated silicon anode (FLG-Si) electrode, as shown in Figure 5c. Due to the introduction of IL electrolyte, the passive layer formation on the anode surface is controlled and enhanced the capacity of the system drastically with a maximum of 4000 mAh g −1 .

Ionic Liquid-Incorporated Solid Polymer Electrolytes
The bid of ILs to LIBs are not limited only for liquid and gel polymer electrolytes, and recently it has been widely constructed using solid polymer electrolyte. Unfortunately, the performance of the LIBs is restricted by the poor room temperature conductivity of solid polymer electrolytes, due to the crystallinity of polymers, which resulted in the decrement of migration rate of lithium ion species to the host matrix. This observation was evidenced by various results reported earlier [41,57,[139][140][141]. The PEO-built solid electrolytes displayed an appropriate conductivity value (10 −4 S cm −1 ) for commercial LIB usage only after their crystalline temperature (Tm); in this case, the amorphous domains are dominant, which permits lithium ions to perceive a greater number of lithium charge carriers [41,120,[142][143][144]. Thus, many attempts have been made, aiming to reduce the crystallinity, as well as to improve the robustness and conductivity in solid polymer electrolytes, which include blended matrices, branched hosts, bulky anionic lithium salts, and the incorporation of additives, such as fillers and plasticizers [145][146][147][148]. One such widely used facile method is to incorporate ILs into the polymer electrolytes, and it has been efficaciously demonstrated in recent years [22,43,85,102].
Recently, the incorporation of RTILs in polymer matrices has attracted considerable attention for their use as solid polymer electrolytes in rechargeable LIBs [24,37]. For instance, the PEO-based solid polymer electrolytes' (SPEs) properties are hindered by the ILs' addition in many ways. The major mechanism behind this phenomenon is explained as follows: the bigger anionic salts have the tendency to weaken the cations interaction from the ether oxygen coordination. The anions in ILs speed up the ionic migration, while the bulky cations are responsible for ionic conduction by means of creating unrestricted volume nearby the polymer lattice. Furthermore, the physical properties of

Ionic Liquid-Incorporated Solid Polymer Electrolytes
The bid of ILs to LIBs are not limited only for liquid and gel polymer electrolytes, and recently it has been widely constructed using solid polymer electrolyte. Unfortunately, the performance of the LIBs is restricted by the poor room temperature conductivity of solid polymer electrolytes, due to the crystallinity of polymers, which resulted in the decrement of migration rate of lithium ion species to the host matrix. This observation was evidenced by various results reported earlier [41,57,[139][140][141]. The PEO-built solid electrolytes displayed an appropriate conductivity value (10 −4 S cm −1 ) for commercial LIB usage only after their crystalline temperature (T m ); in this case, the amorphous domains are dominant, which permits lithium ions to perceive a greater number of lithium charge carriers [41,120,[142][143][144]. Thus, many attempts have been made, aiming to reduce the crystallinity, as well as to improve the robustness and conductivity in solid polymer electrolytes, which include blended matrices, branched hosts, bulky anionic lithium salts, and the incorporation of additives, such as fillers and plasticizers [145][146][147][148]. One such widely used facile method is to incorporate ILs into the polymer electrolytes, and it has been efficaciously demonstrated in recent years [22,43,85,102].
Recently, the incorporation of RTILs in polymer matrices has attracted considerable attention for their use as solid polymer electrolytes in rechargeable LIBs [24,37]. For instance, the PEO-based solid polymer electrolytes' (SPEs) properties are hindered by the ILs' addition in many ways. The major mechanism behind this phenomenon is explained as follows: the bigger anionic salts have the tendency to weaken the cations interaction from the ether oxygen coordination. The anions in ILs speed up the ionic migration, while the bulky cations are responsible for ionic conduction by means of creating unrestricted volume nearby the polymer lattice. Furthermore, the physical properties of the ILs, such as dielectric constant and viscosity, play a key role in electrolyte chemistry, which are the deciding factors for changing the physicochemical and electrical properties of the electrolyte films. The lower viscosity of the ILs and the higher flexibility in the polymer strand chain are increasing the conductivity rate in LIBs. Conversely, the higher dielectric constant value of ILs enhances the dissociation of paired ions, thereby increasing the mobile labile ions, which in turn favors the conductivity enhancement. A typical example of a PEO-based SPE comprising of a low viscosity (65 cP) and high dielectric constant (15) IL, namely EMImTf, in a PEO-LiTf complex has shown an extraordinary thermal stability (380 • C) and better ionic conductivity (3.1 × 10 −4 S cm −1 ) due to the incorporation of low viscous IL [143].
A new class of IL, PYR 14 TFSI in a PEO matrix, subsequently enhances the chemical and electrochemical properties of SPEs [55], which are capable of providing the theoretical capacity (170 mA h g −1 ) at 30 • C through excellent cyclability. In a similar fashion, ILs, like PYR 14 TFSI, Im 13 TFSI, DEME-TFSI and PP 13 -TFSI, Im 13 TFSI, Im 23 PF 6 , etc., have been extensively studied and characterized for SPEs in LIB applications using PEO as the host polymer matrix [20,30,79,116,120,[149][150][151][152]. Apart from PEOs, SPEs containing other polymer hosts have also been extensively studied [98,139,153]. A new class of SPE membranes, comprising IL PYR 1201 TFSI, BEMA and PEGMA, were prepared by the UV-induced photo-polymerization process, which showed a high anodic breakdown voltage of 4.6 V greater than Li/Li + [33]. On the other hand, the electrochemical properties of the SPEs were enhanced with increasing concentration of PYR 14 TFSI and silicon fiber in the polycarbonate matrices. The tremendous increment was observed in lithium transference number (0.36), mechanical robustness, and cycling stability of these poly-carbonate membranes, which paves the way towards utilization as one of the potential candidates in rechargeable LIBs [154]. Additionally, in recent times, chitosan-based SPEs with fifteen different types of ILs were studied and identified as promising separators for LIBs [155]. Recently, polymeric IL (PoIL)-based SPEs have received great attention because of their chemical affinity which results in a compatible combination of stable polymer electrolytes. Li et al. [39,156,157] have prepared a series of SPE membranes containing different anions of guanidium protic ionic liquid (PIL), and it has possessed better thermal stability, with a decomposition temperature of 353 • C, and achieved the conductivity of 1.35×10 −4 S cm −1 at 303 K. Likewise, poly((4-vinyl benzyl)trimethylammonium bis(trifluoro-methanesulfonamide))-based PILs have also been investigated in the recent years [154,155].

Ionic Liquid-Based Ionogel Electrolytes
Immobilizing ILs within organic, inorganic, or hybrid porous matrices lead to a solid-state ion-conducting ionogel system. The crucial role of ILs in ionogel system is maintaining their liquid dynamics, which is accountable for the ion conduction and electrochemical behavior, whereas the porous matrices offer abundant channels to confine the ILs and responsible for mechanical and optical properties.
Recently, solid-state lithium ion batteries with a new class of ionogel electrolytes using non-aqueous sol-gel synthesis based on a tetrabutyl titanate (TBOT) in an alkyl imidazolium IL like Im 13 BF 4 and Im 13 TFSI have explored. They have reported a maximum room temperature ionic conductivity of 10 −3 S cm −1 , which is almost the same order as that is offered by organic liquid electrolytes and ILs [11]. Furthermore, the ionogel electrolytes were stable for long-time use more than one year, without any phase separation, and attained the highest specific capacity of 162 mA h g −1 at 1 C rate [98].
The non-aqueous sol-gel synthesis of ionogel electrolytes is schematically displayed in Figure 6a-d [158], and those prepared ionogel electrolytes delivered the capacity of 153.7 mAh g −1 .
The ILs with epoxy modified silanes formed organically modified silica-tethered solid state ionogels, which have superior ion-conducting and mechanical properties than to conventional solid polymer electrolytes. The synthesis process is exactly matched with the synthesis process of cross-linked gel polymer electrolytes using PVdF-co-HFP as polymer host reported earlier [159]. It is schematically represented in Figure 6e. It is important to notice that the difference between ionogel and GPEs is the host matrix; in the case of GPEs, the polymer acts as host, whereas, the case of ionogel electrolytes generally prefers siloxanes, epoxy, or silane scaffolds, which have been used. For instance, the recent report on 3-glycidyloxypropyltrimethoxy silane with PYR 13 TFSI/LiTFSI ionogel electrolyte has offered 1.91 × 10 −3 S cm −1 at 303 K with a stability window of 4 V [158].  Tan et al. employed ionogel electrolyte (BMImTFSI as the IL, LiTFSI as salt, HCOOH as the cross-linking agent and TEOS as the mesoporous matrices) for LIBs [160] in order to improve battery safety and cycle life. They assembled and fabricated the coin cells with two different approaches. The first approach involves the conventional method of battery assembly by the way of stacking the as prepared ionogel electrolyte on cathodes (they used three different electrodes, such as LiCoO2, LiNi1.5Mn0.5O2, and LiFePO4), followed by lithium metal anode to form a half cell. The second approach involves the inkjet printing of ionogel solvent precursors onto the as-prepared anodes and cathodes, stacked face to face in a coin cell to form a solid-state full cell. The resultant cell was then aged at 35 ºC for 24 h. In these two approaches, they analyzed the electrochemical and cycling performances both conventional (Figure 7a-f) and inkjet-printed electrolyte embedded cells (Figure  7g-l). The fuel cells prepared by ink jet printing show superior performance as compared to conventional half cells due to their better structure stability and interface compatibility between electrode and electrolyte. Hence, this approach of printing ionogel electrolytes onto the electrode surface allows fabrication of high-performance solid-state batteries with improved cycle performance and safety. Tan et al. employed ionogel electrolyte (BMImTFSI as the IL, LiTFSI as salt, HCOOH as the cross-linking agent and TEOS as the mesoporous matrices) for LIBs [160] in order to improve battery safety and cycle life. They assembled and fabricated the coin cells with two different approaches. The first approach involves the conventional method of battery assembly by the way of stacking the as prepared ionogel electrolyte on cathodes (they used three different electrodes, such as LiCoO 2 , LiNi 1.5 Mn 0.5 O 2 , and LiFePO 4 ), followed by lithium metal anode to form a half cell. The second approach involves the inkjet printing of ionogel solvent precursors onto the as-prepared anodes and cathodes, stacked face to face in a coin cell to form a solid-state full cell. The resultant cell was then aged at 35 ºC for 24 h. In these two approaches, they analyzed the electrochemical and cycling performances both conventional (Figure 7a-f) and inkjet-printed electrolyte embedded cells (Figure 7g-l). The fuel cells prepared by ink jet printing show superior performance as compared to conventional half cells due to their better structure stability and interface compatibility between electrode and electrolyte.
Hence, this approach of printing ionogel electrolytes onto the electrode surface allows fabrication of high-performance solid-state batteries with improved cycle performance and safety.
Earlier, a practical methodology employed for the enhancement of lithium mobility in boronic-ionogel electrolytes was using a highly soluble and crosslinkable boron allyl-oxide precursor as a chelating agent and the IL electrolyte solution PYR 14 TFSI/LiTFSI in the PEGDMA. The introduction of a boronic crosslinker in boronic ionogel electrolytes enhanced the lithium ion mobility more significantly than the ionogels fabricated without the boronic cross-linker, which leads to promising LIB performance, including both rate and cyclability, at elevated temperatures [161]. Earlier, a practical methodology employed for the enhancement of lithium mobility in boronic-ionogel electrolytes was using a highly soluble and crosslinkable boron allyl-oxide precursor as a chelating agent and the IL electrolyte solution PYR14TFSI/LiTFSI in the PEGDMA. The introduction of a boronic crosslinker in boronic ionogel electrolytes enhanced the lithium ion mobility more significantly than the ionogels fabricated without the boronic cross-linker, which leads to promising LIB performance, including both rate and cyclability, at elevated temperatures [161]. Polymer-supported ionogels have been hampered by two vital issues, which include the immiscibility between polymers and ILs and loss of the solid-state configuration of the polymers due to high loading of the ILs in polymers. These obstacles were overcome by preparing polymer-immobilized ionogel electrolytes with the mechanochemical activation process. A typical example would be an ionogel with a PEO scaffold and PYR14TFSI percolating phase investigated and observed at the maximum lithium ion conductivity of 7.28 × 10 −4 S cm −1 without any conductivity decay over a long period of time [162]. A mixture of ILs, comprised of EMImTFSI and 3P(Im14TFSI) in PVdF-co-HFP electrospun films gave solid-like composite ionogel electrolytes and showed considerable tensile stability of 8.6 MPa and excellent thermal stability of 370 °C, which can fulfill the main prerequisite for safer energy storage devices, especially in LIBs [1]. Polymer-supported ionogels have been hampered by two vital issues, which include the immiscibility between polymers and ILs and loss of the solid-state configuration of the polymers due to high loading of the ILs in polymers. These obstacles were overcome by preparing polymer-immobilized ionogel electrolytes with the mechanochemical activation process. A typical example would be an ionogel with a PEO scaffold and PYR 14 TFSI percolating phase investigated and observed at the maximum lithium ion conductivity of 7.28 × 10 −4 S cm −1 without any conductivity decay over a long period of time [162]. A mixture of ILs, comprised of EMImTFSI and 3P(Im 14 TFSI) in PVdF-co-HFP electrospun films gave solid-like composite ionogel electrolytes and showed considerable tensile stability of 8.6 MPa and excellent thermal stability of 370 • C, which can fulfill the main prerequisite for safer energy storage devices, especially in LIBs [1].

Ionic Liquid-Based Electrolytes for Supercapacitor Applications
Ever increasing energy demand, depleting resources of fossil fuels, and increasing concern of climate change has motivated researchers to come out with greener and economically viable high-performance options for energy harvesting and storage devices [163][164][165][166][167][168][169][170][171]. Electrochemical energy and related technologies, which converts chemical energy into electrical energy without pollution, seems to be one of the effective way to address this problem. In recent times, SCs have demonstrated several promising characteristics, such as the capability of yielding high power, durable cycle life, and operational safety, and it is considered a next generation energy storage device.
Based on the charge storage mechanism, the two types of SC are: (1) the electrical double layer capacitor (EDLC), where the charge growth occurs at the interface between electrode and electrolyte; and (2) the pseudocapacitor, which uses quick and reversible redox reactions over the electrodes surface. To carry out these functions smoothly, most of the time, carbonaceous materials like carbon black, carbon nanotubes (CNTs), graphene, and activated carbon are employed as electrodes in EDLCs, while, in the case of pseudocapacitors, transition metal compounds (metal oxide) and/or conducting polymers are preferred to be used as electrode materials over the other materials [171][172][173]. EDLCs are having high rate charging-discharging capabilities in addition to high power density, superseding to batteries and fuel cells. In the EDLC, there is electrostatic adsorption of ionic species at the interface of electrode and solution. This leads to the formation of an electrochemical double layer, which ensures no redox reaction during the charging or discharging of these devices.
Among the various parameters, physical and chemical properties of electrolytes are one of the crucial factors to evaluate the performances of SCs. Efficient tuning of these properties is necessary to fabricate capable SCs. In general, aqueous electrolytes (e.g., H 2 SO 4 , KOH, Na 2 SO 4 ) restricts the potential window, which is bounded by the cell voltage, energy, and electric power density. Although replacing these aqueous electrolytes by some organic and natural solvents ensures more stability over the wide range of potential, it certainly raised the issue of operational safety. Organic solvents are flammable, volatile, and sometimes even toxic, which can caused severe health issues. Consequently, the discovery of a more appropriate electrolyte is of massive importance to optimize the efficiency of SCs [4,174]. ILs, which have distinctive properties, like excellent thermal and chemical stabilities, wide electrochemical voltage window, reliable ionic conductivity, non-volatility, and nontoxicity, have been employed to overcome most of the problems associated with usage of liquid and organic electrolytes in SCs [17,175]. In the following sections, special focus is paid to the advances in IL-based electrolytes for applications in SCs. In addition, a detailed investigation is performed on the enhancement of electrochemical properties using IL electrolytes and polymer hybrid electrolytes, which are compared to other organic/aqueous electrolytes with energy storage devices in mind.

Pristine Ionic Liquids as Electrolytes
To realize the dream of greener and economically viable high-performance energy storage devices, a lot of efforts have been taken in designing and developing a new class of materials and technologies [4,176,177]. ILs have tunable physical and chemical properties; henceforth, it has a significant impact on the several of energy harvesting and storage-related technologies. As discussed in the previous section of this review, ILs are molten organic salts with melting points underneath 100 • C. It is observed that most of these IL salts have strong electrostatic forces between their molecular ions. As a result, most of them have low volatility/flammability and high chemical and electrochemical stabilities. These properties, along with high intrinsic ionic conductivity, are highly desirable as solvents and electrolytes for SCs. Earlier results suggested that the capacitance retention and operational safety at high temperatures is much better for SCs with ILs as electrolytes than those using non-aqueous electrolytes [11,25,75,[178][179][180][181][182][183][184][185][186][187][188]. It is also observed that SCs fabricated using ILs can be operated at high cell voltage, which helps the improvement of energy density of SCs to the extent of secondary batteries [180][181][182][183][184][185][186][187][188][189][190][191][192][193].
ILs can be arranged into two groups: protic ILs (PILs) and aprotic ILs (AILs). Significantly, PILs are comprised of equimolar Bronsted acids and Bronsted bases. The proton exchange, from acid to base, makes proton donor and acceptor areas, which, in turn, can prompt the arrangement of H-bonds. PILs are simpler to blend, less expensive, less viscous, and have higher conductivities than AILs [65].
Timperman et al. [65] prepared phosphonium PIL [Bu 3 HP][BF 4 ] and investigated as the electrolyte for carbon-SCs. Kuring et al. [189] investigated a series of different types of ILs, such as Im 13 cation and BF 4 , TCB, TFSI, FSI, and SCN anions, as electrolytes in asymmetric SC cells. They observed the IL electrolytes have a wide electrochemical stability window and better capacitance performance than organic electrolytes. Denshchikov et al. [190] fabricated an SC device using nanostructured carbon electrodes and solvent-free IL 1Me 3 BuImBF 4 as electrolytes with the extreme specific capacitance of 111 F/g at ambient temperature. Shaikh et al. [191] fabricated inexpensive and nontoxic Ru-doped CuO film as an electrode and Bronsted acid, 1-butyl-3-methylimidazolim bisulfite (Im 14 HSO 4 ) as an electrolyte for SCs. In addition, they achieved the capacitance of 406 F.g −1 at low scan rate for 15 volume percentage Ru-doped CuO film. Anouti et al. [192] investigated the two PILs, such as pyrrolidinium methanesulfonate, PYRMeSO 3 , and diisoprpylethylammonium methanesulfonate (DIPEAMeSO 3 ), in the water mixture as the electrolytes with activated carbon as electrodes and observed the specific capacitance of 97 F g −1 with the specific power of 13.9 kW kg −1 at a high current density of 15 A g −1 .
In addition, Maiti et al. [193] used IL Et 4 NBF 4 electrolyte soaked separator between the montmorillonite K10 clay-MWCNT-MnO 2 composite electrodes and achieved 171 W h kg −1 and 96.4 kW kg −1 as the energy and power densities, respectively, which is represented in Figure 8a-e. The acid-base interactions of K10 via its surface OH groups with the IL electrolyte (C 2 H 5 ) 4 N + or TEA + could be the possible reason for observed high performance of EDLC.
In general, as acetonitrile is a preferred solvent for electrolytes which has low viscosity and high conductivity with the mixture of salts: however, it possesses the issue of operational safety owing to their high volatility and flammability. Abdallah et al. [194] successfully replaced aprotic tetraethylammonium tetrafluoroborate (Et 4 NBF 4 ) ILs-acetonitrile in SC applications and proved their less volatile and flammable nature, which may be due to the presence of solvates. Reduced graphene oxide (RGO)-based SCs were fabricated by Chen et al. [195] using IL electrolytes of Im 14 PF 6 and Im 14 BF 4 . They were observed the specific capacitance of 74 F g −1 for the fabricated SC with RGO in Im 14 BF 4 at 10 mV s −1 , which is much better than the specific capacitance of 45 F g −1 for SC with RGO in Im 14 PF 6 .
Demarconnay et al. [15] demonstrated the SCs using PYRNO 3 -based electrolytes and carbon electrodes with the specific capacitance of 121 and 208 F g −1 for their pH value of 7 and 11, respectively. In this case, the triethylammonium bis(trifluoromethylsufonyl)imide-NEt 3 H TFSI-PIL was employed to broaden the electrochemical window. In addition, Brandt et al. [192] investigated the role of water content in protic IL electrolyte on its performance for SC applications. They found that devices have the excellent stability, even at different temperature range, with the operative voltage of 2.4 V. Furthermore, they observed the pseudocapacitive behavior of an AC (Activated Carbon) electrode in protic IL electrolyte due to the water content. Trigueiro et al. [7] prepared the SC using an RGO as an electrode and PYR 13 TFSI as the electrolyte, which showed the specific capacitance of 71.5 F g −1 at 10 mV s −1 .
The operating potential window, which is generally governed by electrolyte, is one of the important parameter that can affect the specific energy of EDLCs. ILs have been paid attention to as electrolytes for EDLCs because they tend to have comparatively broad potential windows compared to organic electrolytes. The maximum specific energies were attained with IL electrolytes that have reasonable electrochemical stability, low viscosity, small ionic volumes, and therefore high ionic conductivity. Yang et al. [196] studied graphene nanosheets to enhance SC behavior in a butylmethylpyrrolidinium-dicyanamide (PYR 14 DCA) IL electrolyte. Shao et al. [197] utilized IL (EMIMBF 4 ) electrolyte and CNT spaced graphene aerogels electrodes for SCs, which offered the highest capacitance of 183.3 F g −1 at 0.5 A g −1 and the energy density of 80 W h kg −1 . Fuertes et al. [198] fabricated an SC using EMImTFSI as the electrolyte and porous carbon electrode with a specific capacitance of 160 F g −1 at 1 A g −1 .
The operating potential window, which is generally governed by electrolyte, is one of the important parameter that can affect the specific energy of EDLCs. ILs have been paid attention to as electrolytes for EDLCs because they tend to have comparatively broad potential windows compared to organic electrolytes. The maximum specific energies were attained with IL electrolytes that have reasonable electrochemical stability, low viscosity, small ionic volumes, and therefore high ionic conductivity. Yang et al. [196] studied graphene nanosheets to enhance SC behavior in a butylmethylpyrrolidinium-dicyanamide (PYR14DCA) IL electrolyte. Shao et al. [197] utilized IL (EMIMBF4) electrolyte and CNT spaced graphene aerogels electrodes for SCs, which offered the highest capacitance of 183.3 F g −1 at 0.5 A g −1 and the energy density of 80 W h kg −1 . Fuertes et al. [198] fabricated an SC using EMImTFSI as the electrolyte and porous carbon electrode with a specific capacitance of 160 F g −1 at 1 A g −1 .
Kim et al. [187] successfully achieved an ultrahigh energy densities in assembled SCs due to the excellent pore structure of CNF-based electrodes in IL electrolyte systems. Jha et al. [199] reported a specific capacitance of 222 F g −1 for SCs using an IL Im14BF4 electrolyte. Further, the similar type of BF4 anion-based IL electrolyte provides better performance with other carbonaceous materials as reported elsewhere [32,197,[199][200][201].
[DCA] as potential electrolyte for N-rGO aerogel electrodes-based SCs, which delivered the specific capacitance of 764.53 F g−1 at 1 A g −1 . The electrochemical and cycling properties of pristine IL-based electrolytes are tabulated in Table 3 [193]. Copyright 2016 Elsevier.
Kim et al. [187] successfully achieved an ultrahigh energy densities in assembled SCs due to the excellent pore structure of CNF-based electrodes in IL electrolyte systems. Jha et al. [199] reported a specific capacitance of 222 F g −1 for SCs using an IL Im 14 BF 4 electrolyte. Further, the similar type of BF 4 anion-based IL electrolyte provides better performance with other carbonaceous materials as reported elsewhere [32,197,[199][200][201]. Iamprasertkun et al. [6] demonstrated a 1-butyl-1-methylpyrrolidinium dicyanamide, [BMP][DCA] as potential electrolyte for N-rGO aerogel electrodes-based SCs, which delivered the specific capacitance of 764.53 F g−1 at 1 A g −1 . The lectrochemical and cycling properties of pristine IL-based electrolytes are tabulated in Table 3  .  Using Im 14 NTf 2 electrolyte, Bettini et al. [231] assembled the SC with cluster-assembled nanostructured carbon electrodes, which showed the maximum capacitance of 75 F g −1 .
Deng et al. [163] developed the MnO 2 nanowires/Ni foam as an electrode and the new type of lithium-ion quasi-IL (LiClO 4 /2-oxazolidinone (OZO) salts) electrolyte for pseudocapacitors, which operated in the broad potential range (2.5 V) with 304 W h kg −1 energy density. Fu et al. [222] got the capacitance of 132 F g −1 with the specific energy and power density of 143.7 W h kg −1 and 2.8 kW kg −1 , respectively, for IL Im 14 PF 6 in acetonitrile electrolyte. Fuertes et al. [198] studied the effect of Im 14 TFSI at different temperatures using sawdust carbon electrodes, and it showed apparently very good capacitance behavior. Its corresponding CV curves are displayed in Figure 9a-d. Tooming et al. [228] examined the effect of EMImI (5 wt%) on EMImBF 4 as the electrolyte on the electrochemical performances in EDLC. They observed that specific conductivity decreased to 12.8 mS cm −1 from 13.6 mS cm −1 due to the incorporation of 5 wt% EMImI into the EMImBF 4 with the improved melting point of 19.5 • C. Zhang et al. [227] reported the specific capacitance of 523.3 F g −1 at 3 A g −1 with the specific power of 20.4 kW kg −1 at a specific energy of 8.5 W h kg −1 for Im 14 PF 6 /N, N-DMF electrolyte and MnO 2 electrodes. Sathish et al. [225] attained the capacitance of 104 F g −1 using N-doped GN and Im 13 TFSA as the electrode and electrolyte, respectively.
Xie et al. [232] investigated redox-active IL as electrolyte for SC applications where the IL was utilized with ferrocene as an electroactive material to enhance the energy density, which led to high concentrations of redox moieties in the electrolyte (2.5 M) and a wide working potential, around 2.5 V. Lin et al. [233] achieved a highest specific capacitance of 130 F g −1 (63 mA h g −1 ) at −20 • C, 100 F g −1 (49 mA h g −1 ) at −30 • C and 175 F g −1 (85 mA h g −1 ) at 80 • C for fabricated SC using an eutectic mixture of Pip 23 TFSI and PYR 24 TFSI IL electrolyte with graphene film. Tsai et al. [188] employed a eutectic mixture of ILs, such as Pip 13 FSI and PYR 14 FSI, as an electrolyte with exfoliated graphite oxide electrodes, which reached 180 F g −1 in the voltage window of 3.5 V at 20 mV s −1 . Furthermore, various novel ILs, which, comprising different anions, such as BF 4 , triflate, and TFSI, as well as cations, such as ammonium, Im, Pip, PY, and PYR, are used as electrolytes for SCs [8,32,200]. ILs presents a distinctive set of behaviors, which made them promising material for electrochemical SC devices. The development of ILs in SC applications is promising but also presents several challenges.

Ionic Liquid Based Polymer Electrolytes
The liquid electrolytes, including ILs, are capable of the fabrication of SC, but they have limitations due to their requirement of encapsulation, which limits their use in flexible and printed electronics [47]. The IL-based (gel) polymer electrolytes (GPEs) are suitable alternatives to address this issue in IL-based electrolytes for flexible energy storage devices [205]. The incorporation of ILs and their Polymers 2020, 12, 918 20 of 37 associated functional groups (i.e., cations, like pyrrolidinium, pyridinium, and imidazolium; and anions, like triflates, hexafluorophosphate, and tetrafluoroborate) with well-designed polymers are creating a new avenue of materials, which has fascinating properties and suitable for a huge range of applications. By appearing in their chemical structure, IL incorporated polymers are polyelectrolytes with restating polymers group stance as the electrolyte (cation/anion). In GPE, polymeric network ensures mechanical reliability, which makes them more mechanically stable. However, GPE systems which comprised of liquid electrolyte with organic solvent are showed inferior electrochemical stability with narrow potential window and low thermal stability due to the flammable nature of organic solvents [205].
Ujjain et al. [234] assembled a SC with a high specific capacitance of 242 F g −1 at 5 mV s −1 and stability up to 12,000 cycles using modified RGO electrodes with an IL of Im 14 BF 4 and GPE of Im 13 BF 4 /[PVdF-co-HFP] as shown in Figure 9e-h. Tamilarasan et al. [235] fabricated an SC using high strain stretchable IL-integrated Im 14 TFSI/PMMA electrolyte and graphene electrode. Similarly, Lee et al. [236] fabricated as stretchable SC using PVdF-co-HFP/IL electrolyte and PDMS/CNT electrodes. This SC cell possessed superior capacitance retention of 96.6% over 3000 cycles. The PVdF-co-HFP/IL GPE improves the operating potential window and the energy density. In addition, Tamilarasan et al. [122] observed 98 F g −1 of specific capacitance at 10 A g −1 for SC using IL-integrated polymer electrolytes (PAN/Im 1,4 TFSI) with the specific power and energy density of 82 kW kg −1 and 32.3 W h kg −1 , respectively.
Polymers 2020, 12, x FOR PEER REVIEW 20 of 36 solvent are showed inferior electrochemical stability with narrow potential window and low thermal stability due to the flammable nature of organic solvents [205]. Ujjain et al. [234] assembled a SC with a high specific capacitance of 242 F g −1 at 5 mV s −1 and stability up to 12,000 cycles using modified RGO electrodes with an IL of Im14BF4 and GPE of Im13BF4/[PVdF-co-HFP] as shown in Figure 9e-h. Tamilarasan et al. [235] fabricated an SC using high strain stretchable IL-integrated Im14TFSI/PMMA electrolyte and graphene electrode. Similarly, Lee et al. [236] fabricated as stretchable SC using PVdF-co-HFP/IL electrolyte and PDMS/CNT electrodes. This SC cell possessed superior capacitance retention of 96.6% over 3000 cycles. The PVdF-co-HFP/IL GPE improves the operating potential window and the energy density. In addition, Tamilarasan et al. [122] observed 98 F g −1 of specific capacitance at 10 A g −1 for SC using IL-integrated polymer electrolytes (PAN/Im1,4TFSI) with the specific power and energy density of 82 kW kg −1 and 32.3 W h kg −1 , respectively. Figure 9. CV curves of pure EMImTFSI (a,b) and EMImTFSI/acrylonitrile (AN) (c,d) using sawdust carbon symmetrical electrodes at room temperature; CV curves (e) different potential window and (f) different scan rate 10 -500 mV s −1 , (g) capacitance variations with potential window, (h) Arrhenius plot of specific capacitance (Inset: temperature dependent CV curve) for f-graphene in BMImBF4 electrolyte and gel electrolytes [198,234]. Copyright 2017 Elsevier.
Recently, flexible SCs were constructed using CNTs and IL-based GPEs, and their capacitance value was 135 F g −1 at 2 A g −1 [204]. Pandey et al. [5] studied IL Im 13 FAP-incorporated GPEs and MWCNT electrodes for SC applications.

Summary and Outlook
In this review, we outlined the recent developments of liquid, gel, and solid IL-based electrolytes for their applications in LIBs and SCs. In particular, discussions were focused to highlight the excellent electrochemical and physicochemical properties of some organically modified electrolytes with ILs for their applications in energy storage systems. Today, the significance of EES materials is increasing due to their huge requirements. Hence, many new class of ILs and polymeric ILs have been developed for LIBs and SCs that provide high-performance devices with excellent specific capacity and capacity retention properties.
Some of merits associated with the use of ILs for fabricating EES devices are as follows: (a) the characteristic properties of IL, includes thermal stability, ionic conductivity, and negligible vapor pressure certainly matches with the industrial requirements; (b) the low volatility and better electrochemical stability of ILs makes them ideal choice as electrolytes for LIBs and SCs; (c) improved energy density and capacity maintenance, hence making it is the key material for large-scale energy storage systems; and (d) the excellent unique feature of ILs, observed from most of the literature, is its capability to operate at elevated temperatures, which makes them the promising candidates for applications in portable electronic devices and hybrid electric vehicles. Along with the polymer host, ILs can be used to formulate solid and gel electrolytes; hence, it would be a capable material for many applications, like flexible electronics, batteries, wearable, fuel cells, bendable SCs, and DSSCs. Conflicts of Interest: "The authors declare no conflict of interest." "The funders had no role in the design of the study; in the collection, analyses, or interpretation of data; in the writing of the manuscript, or in the decision to publish the results".