Oligoether/Zwitterion Diblock Copolymers: Synthesis and Application as Cathode-Coating Material for Li Batteries

Poly (ethylene oxide) (PEO) has been investigated as an ion-conductive matrix for several decades due to its excellent properties. However, further improvements are needed to enable a PEO-based ion-conductive matrix for practical applications. In order to develop novel solid polymer electrolytes based on zwitterions, we synthesized diblock copolymers (PPEGMA-b-SPBs) with oligoether and zwitterionic side-chains and evaluated their physico-chemical properties. PPEGMA-b-SPBs with various unit ratios were synthesized by RAFT polymerization. PPEGMA-b-SPBs with/without LiTFSA exhibited two distinct glass transition temperatures regardless of the unit ratio of PEGMA and SPB. AFM observations clearly revealed phase-separated structures. The ionic conductivity of PPEGMA-b-SPBs increased even at a high salt concentrations such as [EO]:[Li] = 6:1 and was over 10−5 S cm−1 at 25 °C. This tendency is unusual in a PEO matrix. The oxidation stability of PPEGMA-b-SPBs was about 5.0 V vs. Li/Li+, which is a higher value than that of PEO. The improvement of the electrochemical properties is attributed to the introduction of the SPB block into the block copolymers. PPEGMA-b-SPBs were evaluated as cathode-coating materials for Li batteries. The discharge capacity and coulombic efficiency of the cells employing the cathode (LiNi1/3Mn1/3Co1/3O2 (NMC)) coated with the block copolymers were much higher than those of the cell employing the pristine cathode at the 50th cycle in the cut-off voltage range of 3.0–4.6 V.


Introduction
Poly (ethylene oxide) (PEO) has been investigated as an ion-conductive matrix for several decades due to its excellent properties, such as high polarity to dissociate Li-salts and flexibility to transport Li-ions along the polymer chain [1,2]. The ionic conductivity of PEO-based electrolytes is about 10 −4 S cm −1 at room temperature. PEO can be utilized as a solid electrolyte for rechargeable batteries, e.g., Li-ion batteries. However, further improvements are needed to enable a PEO-based ion-conductive matrix for practical applications. Although an abundance of PEO derivatives have been reported, it is difficult to improve the ionic conductivity of PEO-based electrolytes. This is because the glass transition temperature (T g ) increases and the ionic conductivity decreases as the concentration of Li-salt increases. In other words, there is a trade-off relationship between Li-ion concentration and Li-ion mobility. On the other hand, polycarbonate-based electrolytes have been reported as alternative solid polymer electrolytes [3][4][5]. Their ionic conductivity is about 10 −7 to 10 −3 S cm −1 at 60 • C, and the lithium transport number (t Li+ ) is typically in the range 0.4 to 0.8. Polycarbonate-based electrolytes are fascinating materials as an alternative to PEO, but the oxidation potential is around 3 V [4], which is lower than that of PEO-based electrolytes.
Additives are being actively studied in order to easily improve various properties of PEO. The ionic conductivity and t Li+ of PEO-based electrolytes and resistance at the electrolyte/electrode interface are improved by adding plasticizers [6,7] and inorganic Polymers 2021, 13, 800 2 of 12 fillers [8,9] to PEO-based electrolytes. On the other hand, zwitterions [10][11][12], which have both a cation and anion in the same molecule, have been proposed as new additives. The ionic conductivity and diffusion coefficient of Li-ion in polymer gel electrolytes are improved by the addition of zwitterions [13,14]. Furthermore, such improvements are also observed when zwitterions are added to ionic liquids, and the coulombic efficiency based on the electrochemical redox reaction of Li is improved [15].
The melting points of typical zwitterions are above 100 • C, hence zwitterions are solid at room temperature [11]. Recently, we succeeded in synthesizing zwitterions that are liquid at room temperature [16]. Furthermore, we found that liquid zwitterions improve the electrochemical (oxidation) stability of oligoether compounds [17,18]. Generally, the oxidation potential of PEO-based electrolytes is about 4.0 V vs. Li/Li + [19,20], and cathode active materials such as LiCoO 2 (LCO) and LiNi 1/3 Mn 1/3 Co 1/3 O 2 (NMC) cannot be applied as high potential electrodes in Li-ion batteries with PEO-based electrolytes. Interestingly, when a small amount of zwitterion was added to oligoethers, the oxidation potential of oligoethers was improved to about 5 V. The combination of zwitterion and oligoether is interesting as an electrolyte material. However, oligoether electrolytes are liquids and have the same problems such as liquid leakage and volatility as organic electrolyte solutions. By developing polymer electrolyte membranes, not only can the above problems be solved, but also separator-free batteries can be fabricated. These allow us to develop safe and flexible devices. In order to develop novel solid polymer electrolytes based on zwitterions and oligoethers, we synthesized random copolymers with zwitterionic and oligoether side-chains [21]. Their lithium bis(trifluoromethanesulfonyl)amide (LiTFSA) composites exhibited an ionic conductivity of 10 −4 S cm −1 at 80 • C. Contrary to conventional PEO-based electrolytes, their ionic conductivity was maintained even at high LiTFSA concentration because the high dipole moment of zwitterions leads to a dissociation of LiTFSA through electrostatic interaction [22,23].

Synthesis of PPEGMA-b-SPB
The chain extension of PPEGMA 68 to PPEGMA 68 -b-SPB m was carried out in a similar manner as RAFT polymerization of PPEGMA 68 . These copolymers were referred to as PPEGMA 68 -b-SPB m , where 68 and m represent the number of PEGMA and SPB units in the copolymers, respectively. SPB, PPEGMA 68 (2.00 g, 6.06 × 10 −5 mol) and ACVA (1.4 mg, 5.0 × 10 −6 mol) were dissolved in pure water (18.1 MΩ cm −1 ) 25 mL and placed in dried polymerization tubes. The polymerization mixture was degassed with five pump thaw cycles, and then the tubes were sealed under nitrogen. The polymerization tubes were placed into a shaker at 70 • C. After 15 h, the reaction systems were cooled down in an ice bath. The polymer was purified by dialysis against pure water (18.1 MΩ cm −1 ) and recovered by freeze drying, yielding polymers as pink solids (general yields: 70-80%). 1

Preparation of Neat and Li Composite Films
In an Ar filled globe box, given amounts of PPEGMA 68 -b-SPB m and LiTFSA were dissolved in HFIP, and these mixtures were stirred at 25 • C for 24 h. Then, these solutions were cast on a PTFE plate and were dried at 25 • C for 24 h and 60 • C for 48 h under a nitrogen atmosphere. These films were dried in vacuo at 60 • C for 48 h before use. The LiTFSA concentration was varied from [EO]/[Li] = 6:1 to 24:1.

Methods
1 H NMR measurements were carried out on a Bruker Avance III HD Nanobay 400 NMR spectrometer to confirm the chemical structures of products. Elemental analyses were carried out with a GC elemental analyzer (PE 2400-II, PerkinElmer, Inc. (Waltham, MA, USA)). The molecular weight and molar mass dispersity of PPEGMA 68 were determined with gel permeation chromatography (GPC, PEO/PEG standard, Tosoh Corp. (Yamaguchi, Japan)) using DMF solution with 0.1 wt% LiCl as the eluent (1.0 mL min −1 ) at 40 • C.
The thermal properties were measured by thermogravimetric analysis (TGA; TG-DTA7200, Hitachi High-Tech Corp. (Minato-ku, Tokyo, Japan)). The samples were heated from 25 • C to 500 • C at a scan rate of 10 • C min −1 under a nitrogen atmosphere. The thermal behavior of the samples was measured with differential scanning calorimetry (DSC) (DSC7020, Hitachi High-Technologies Corp.) between −150 and 150 • C at a heating/cooling rate of 10 • C min −1 .
The morphology of the film surface was measured by atomic force microscopy (AFM; SPM-9600, Shimadzu Corp. (Kyoto, Japan)). The AFM images were generated in the tapping mode with an amplitude ratio within 0.90-1.00 to avoid monolayer damage. The AFM cantilevers (NCHR-20, Nanoworld Co., Ltd. (Switzerland)) had spring constants in the range of 42 N m −1 , the scanning range was 1 µm × 1 µm and the scanning rate was 1.0 Hz.
The ionic conductivity values of the samples were obtained by measuring the complex impedance between 100 mHz and 1 MHz (applied voltage: 10 mV) using an impedance analyzer (VSP-300, BioLogic (France)) over the temperature range of −40 to 100 • C. The temperature was controlled using a constant-temperature oven (SU-262, Espec Corp. Kitaku, Osaka, Japan). A stainless steel cell (TYS-00DM01, Toyo System Co., Ltd. (Fukushima, Japan)) was used. Two platinum plates polished with 1.0, 0.3, and 0.05 µm Al 2 O 3 powder were used as the electrode. The AC impedance method was used to analyze the ionic conductivity of the block copolymers at various temperatures. The ionic conductivity of the electrolytes was determined using where σ represents ionic conductivity, R is the intercept at the real axis in the impedance Nyquist plot, S is the geometric area of the electrolyte-electrode interface, and d is the distance between the two electrodes. Cyclic voltammetry measurements (CV; VSP-300, BioLogic (France)) were carried out in the potential range of −0.25 and 1.0 V at 60 • C at a scan rate of 1.0 mV s −1 with lithium foils as the reference and counter electrodes. A stainless steel cell (TYS-00DM01, Toyo System Co., Ltd. (Fukushima, Japan)) was used as the CV measurement cell. A nickel plate polished with 1.0, 0.3, and 0.05 µm Al 2 O 3 powder was used as the working electrode. Linear sweep voltammetry (LSV) measurements (VSP-300, BioLogic (France)) were carried out in the potential range of 3.0 to 6.0 V at 60 • C at a scan rate of 1.0 mV s −1 . Lithium foils were used as the reference and counter electrodes, while platinum plates were used as working electrodes in the potential ranges of 3.0 to 6.0 V. NMC (85 wt%), AB (6 wt%), and PVDF (9 wt%) were mixed in N-methylpyrrolidone, then the composite solution was cast on the current collector, aluminum foil. The coated aluminum foils were dried at 80 • C for 1 h and were pressed at 6 MPa and 70 • C for 1 h. The coated aluminum foils were used as the pristine cathode. For application to cathode-coating material, PPEGMA 68 -b-SPB 121 was applied onto the cathode. PPEGMA 68 -b-SPB 121 /HFIP solution (10 mg mL −1 ) was prepared. Spin coating (1H-D7, Mikasa (Minato-ku, Tokyo, Japan) was used for the fabrication of thin films to deposit a uniform coating of the block copolymer on the cathode surface and was performed at 3000 rpm for 30 s. The coated cathodes were dried at 60 • C for 48 h. Lithium foils were used as the anode.

Synthesis of Oligoetehr/Zwitterion Diblock Copolymers
A homopolymer of PEGMA, PPEGMA was synthesized by RAFT polymerization in 1,4-dioxane. The number-average molar mass (M n ) and mass-average molar mass (M w ) were determined by GPC measurements to be 33,000 and 35,300 g mol −1 , respectively. The molar mass dispersity (Ð M ) was calculated from the molecular weight values to be 1.07, indicating that the molecular weight of PPEGMA is well-controlled by RAFT polymerization. The polymerization degree (n) of PPEGMA n was also calculated from the M n value to be 68. Figure  The coated cathodes were dried at 60 °C for 48 h. Lithium foils were used as the anode.

Synthesis of Oligoetehr/Zwitterion Diblock Copolymers
A homopolymer of PEGMA, PPEGMA was synthesized by RAFT polymerization in 1,4-dioxane. The number-average molar mass (Mn) and mass-average molar mass (Mw) were determined by GPC measurements to be 33,000 and 35,300 g mol −1 , respectively. The molar mass dispersity (ÐM) was calculated from the molecular weight values to be 1.07, indicating that the molecular weight of PPEGMA is well-controlled by RAFT polymerization. The polymerization degree (n) of PPEGMAn was also calculated from the Mn value to be 68. Figure 1a shows the 1 H NMR spectrum of PPEGMA68 in D2O. The chemical shifts of the methacrylate group were observed at about 1.0 and 2.0 ppm. The chemical shifts, which are assigned to the oligoether side-chain of PEGMA, were observed in the range of 3.0 to 4.0 ppm. These results confirm the successful synthesis of PPEGMA. We synthesized four kinds of diblock copolymers, PPEGMA68-b-SPBm, with various SPB unit numbers as summarized in Table 1. The number-averaged molar mass (Mn) of PPEGMA68-b-SPBm was determined by 1 H NMR measurements to be in the range of 37,800 and 67,000 g mol −1 . Figure 1b shows the 1 H NMR spectrum of PPEGMA68-b-SPB121 in D2O. The chemical shifts of the zwitterionic side-chain were observed in the range of 2.2 to 4.0 ppm. From these results, the block copolymers composed of PEGMA and SPB were successfully obtained by RAFT polymerization. The SPB unit numbers (m) were calculated from the Mn values of diblock copolymers and were in the range of 17 and 121. The ratio of m and n (m/n) was determined to be from 0.25 to 1.8. We synthesized four kinds of diblock copolymers, PPEGMA 68 -b-SPB m , with various SPB unit numbers as summarized in Table 1. The number-averaged molar mass (M n ) of PPEGMA 68 -b-SPB m was determined by 1 H NMR measurements to be in the range of 37,800 and 67,000 g mol −1 . Figure 1b shows the 1 H NMR spectrum of PPEGMA 68 -b-SPB 121 in D 2 O. The chemical shifts of the zwitterionic side-chain were observed in the range of 2.2 to 4.0 ppm. From these results, the block copolymers composed of PEGMA and SPB were successfully obtained by RAFT polymerization. The SPB unit numbers (m) were calculated from the M n values of diblock copolymers and were in the range of 17 and 121. The ratio of m and n (m/n) was determined to be from 0.25 to 1.8.

Thermal Properties
DSC measurements were performed on the diblock copolymers in order to detemine the thermal properties. Figure 2 shows (a) DSC curves of neat diblock copolymers, PPEGMA 68 -b-SPB m , and (b) PPEGMA 68 -b-SPB 121 /LiTFSA composites at the 2nd heating scan. All the neat diblock copolymers exhibited two distinct glass transition temperature (T g ) values at around −75 and 5 • C as shown in Figure 2a. The T g values are also summarized in Table 1. The lower T g (T g,L ) is almost the same with the T g (−74 • C) of PPEGMA [29]. Galin et al. reported that a random copolymer composed of butyl acrylate and zwitterionic monomer exhibited two distinct T g values at −38 and 44 • C, which corresponded to buryl acrylate and zwitterion, respectively [23]. The lower T g and higher T g should be based on PEGMA and SPB units, respectively. Both T g , L and T g , H exhibited almost the same values regardless of the unit ratio, m/n. These results indicate that PPEGMA and SPB are incompatible components and tend to spontaneously form phase-separated structures. AFM observation was performed to investigate phase-separated structures for PPEGMA 68 -b-SPB m . Microphase separation was observed for all the block coplymers (data not shown). The SPB block formed an aggregation in the matrix due to strong interaction between zwitterionic side-chains.

Thermal Properties
DSC measurements were performed on the diblock copolymers in order to detemine the thermal properties. Figure 2 shows (a) DSC curves of neat diblock copolymers, PPEGMA68-b-SPBm, and (b) PPEGMA68-b-SPB121/LiTFSA composites at the 2nd heating scan. All the neat diblock copolymers exhibited two distinct glass transition temperature (Tg) values at around −75 and 5 °C as shown in Figure 2a. The Tg values are also summarized in Table 1. The lower Tg (Tg,L) is almost the same with the Tg (−74 °C) of PPEGMA [29]. Galin et al. reported that a random copolymer composed of butyl acrylate and zwitterionic monomer exhibited two distinct Tg values at −38 and 44 °C, which corresponded to buryl acrylate and zwitterion, respectively [23]. The lower Tg and higher Tg should be based on PEGMA and SPB units, respectively. Both Tg,L and Tg,H exhibited almost the same values regardless of the unit ratio, m/n. These results indicate that PPEGMA and SPB are incompatible components and tend to spontaneously form phase-separated structures. AFM observation was performed to investigate phase-separated structures for PPEGMA68-b-SPBm. Microphase separation was observed for all the block coplymers (data not shown). The SPB block formed an aggregation in the matrix due to strong interaction between zwitterionic side-chains.  respectively. The T g , H of PPEGMA 68 -b-SPB 121 /LiTFSA was lower than that of the neat block copolymer. A low molecular weight zwitterion, 4-(1-ethyl-1H-imidazol-3-ium-3yl)butane-1-sulfonate, exhibits a T g at 18 • C. Interestingly, the equimolar mixture of the zwitterion and LiTFSA forms a liquid at room temperature and exhibits a T g at −37 • C [11]. The aggregation state of the SPB block will be plasticized by the addition of LiTFSA.

Surface Morphology
The surface morphology was investigated by AFM measurements for PPEGMA 68 -b-SPB 121 with various LiTFSA concentrations ([EO]:[Li] = 6:1, 12:1, 18:1, and 24:1). Figure 3 shows AFM (a) height and (b) phase images of PPEGMA 68 -b-SPB 121 /LiTFSA composites. Phase-separated structures were observed for both height and phase images of all the composites. In the AFM height images, round dark domains are the SPB block according to the volume ratio of SPB block and PEGMA block. The number of the round dark domains decreased with increasing LiTFSA concentration. In addition, the surface roughness decreased with increasing LiTFSA concentration. The AFM phase images also showed the same phase-separated structure as the height images. The aggregation of SPB block was observed as round bright domains in the phase images. The number of round bright domains decreased with increasing LiTFSA concentration. These results suggest that the SPB block was plasticized by the addition of LiTFSA, and the phase-separated structure was relaxed due to the mixture formation of SPB and PEGMA blocks. This tendency is in good accordance with the results of thermal properties. The Tg,H of PPEGMA68-b-SPB121/LiTFSA was lower than that of the neat block copolymer. A low molecular weight zwitterion, 4-(1-ethyl-1H-imidazol-3-ium-3-yl)butane-1-sulfonate, exhibits a Tg at 18 °C. Interestingly, the equimolar mixture of the zwitterion and LiTFSA forms a liquid at room temperature and exhibits a Tg at −37 °C [11]. The aggregation state of the SPB block will be plasticized by the addition of LiTFSA.

Surface Morphology
The surface morphology was investigated by AFM measurements for PPEGMA68b-SPB121 with various LiTFSA concentrations ([EO]:[Li] = 6:1, 12:1, 18:1, and 24:1). Figure 3 shows AFM (a) height and (b) phase images of PPEGMA68-b-SPB121/LiTFSA composites. Phase-separated structures were observed for both height and phase images of all the composites. In the AFM height images, round dark domains are the SPB block according to the volume ratio of SPB block and PEGMA block. The number of the round dark domains decreased with increasing LiTFSA concentration. In addition, the surface roughness decreased with increasing LiTFSA concentration. The AFM phase images also showed the same phase-separated structure as the height images. The aggregation of SPB block was observed as round bright domains in the phase images. The number of round bright domains decreased with increasing LiTFSA concentration. These results suggest that the SPB block was plasticized by the addition of LiTFSA, and the phase-separated structure was relaxed due to the mixture formation of SPB and PEGMA blocks. This tendency is in good accordance with the results of thermal properties.

Ionic Conductivity
The effect of the unit number of SPB on the ionic conductivity was investigated for PPEGMA68-b-SPBm (m = 17, 31, 62, and 121). The Li-salt concentration was fixed at [EO]:[Li] = 6:1. Figure 4a shows the Arrhenius plots of ionic conductivities for PPEGMA68b-SPBm/LiTFSA composites. The temperature dependence of ionic conductivities exhibited upper convex curves for all PPEGMA68-b-SPBm/LiTFSA composites, suggesting that the ion motion in the block copolymers is mainly coupled with the segmental motion of PPEGMA matrix, which is the typical ion conduction mechanism in a PEO matrix [1,2]. The ionic conductivities of PPEGMA68-b-SPB17 and PPEGMA68-b-SPB31 were almost the same within the temperature range measured in this study. The two block copolymers exhibited the highest ionic conductivity at higher temperatures above 60 °C in this study. On the other hand, at lower temperatures below 60 °C, the ionic conductivity of block copolymers increased with increasing the unit number of SPB. The ionic conductivity is governed by the number of carrier ions and carrier ion mobility. This tendency would

Ionic Conductivity
The effect of the unit number of SPB on the ionic conductivity was investigated for PPEGMA 68 -b-SPB m (m = 17, 31, 62, and 121). The Li-salt concentration was fixed at [EO]:[Li] = 6:1. Figure 4a shows the Arrhenius plots of ionic conductivities for PPEGMA 68b-SPB m /LiTFSA composites. The temperature dependence of ionic conductivities exhibited upper convex curves for all PPEGMA 68 -b-SPB m /LiTFSA composites, suggesting that the ion motion in the block copolymers is mainly coupled with the segmental motion of PPEGMA matrix, which is the typical ion conduction mechanism in a PEO matrix [1,2]. The ionic conductivities of PPEGMA 68 -b-SPB 17 and PPEGMA 68 -b-SPB 31 were almost the same within the temperature range measured in this study. The two block copolymers exhibited the highest ionic conductivity at higher temperatures above 60 • C in this study. On the other hand, at lower temperatures below 60 • C, the ionic conductivity of block copolymers increased with increasing the unit number of SPB. The ionic conductivity is governed by the number of carrier ions and carrier ion mobility. This tendency would result in the enhancement of Li-salt dissociation by SPB units, which has high polarity [22,23]. As a result, a large number of carrier ions is provided into the block copolymer matrix. Thus, PPEGMA 68 -b-SPB 121 , which has a longer SPB block, exhibited higher ionic conductivity than those of the other block copolymers especially at lower temperature range below 60 • C. In other words, PPEGMA 68 -b-SPB 121 exhibited a gentle slope (lower activation energy) for the Arrhenius plot of ionic conductivity, suggesting that the polarity of the zwitterion structure prevents the aggregation of dissociated ions by the enhancement of Li-salt dissociation.
Polymers 2021, 13, x 8 of 12 result in the enhancement of Li-salt dissociation by SPB units, which has high polarity [22,23]. As a result, a large number of carrier ions is provided into the block copolymer matrix. Thus, PPEGMA68-b-SPB121, which has a longer SPB block, exhibited higher ionic conductivity than those of the other block copolymers especially at lower temperature range below 60 °C. In other words, PPEGMA68-b-SPB121 exhibited a gentle slope (lower activation energy) for the Arrhenius plot of ionic conductivity, suggesting that the polarity of the zwitterion structure prevents the aggregation of dissociated ions by the enhancement of Li-salt dissociation.  [3,30] because the introduction of a large amount of Li-salt into the PEO matrix induces an increase in Tg, namely, the decrease in segmental motion of PEO matrix, which results in the decrease in ionic conductivity. PPEGMA68-b-SPB121/LiTFSA composites exhibited an unusual tendency for Li-salt concentration dependence on ionic conductivity. This is attributed to the high polarity of the zwitterion structure in the SPB units enhancing the Li-salt dissociation (vide supra).

Electrochemical Properties
The electrochemical stability of electrolyte materials is an important factor in determining the battery performance. To determine the effect of the SPB block on the electrochemical stability of the diblock copolymers, linear sweep voltammetry (LSV) measurements were carried out at 60 °C. Figure 5a shows the LSV results of PPEGMA68/LiTFSA and PPEGMA68-b-SPB121/LiTFSA (anodic scan from 2.9 to 5.6 V). The oxidation potential of PPEGMA was approximately 4.2 V vs. Li/Li + , which is identical to the value reported previously for PEO-based electrolytes [31]. On the other hand, the oxidation potential of PPEGMA68-b-SPB121 was approximately 5.0 V vs. Li/Li + . The oxidation limit was improved from 4.2 to 5.0 V by the introduction of SPB block in the copolymer. We have already reported that the oxidation limit of oligoether electrolytes is improved from around 4.5 to  [3,30] because the introduction of a large amount of Li-salt into the PEO matrix induces an increase in T g , namely, the decrease in segmental motion of PEO matrix, which results in the decrease in ionic conductivity. PPEGMA 68b-SPB 121 /LiTFSA composites exhibited an unusual tendency for Li-salt concentration dependence on ionic conductivity. This is attributed to the high polarity of the zwitterion structure in the SPB units enhancing the Li-salt dissociation (vide supra).

Electrochemical Properties
The electrochemical stability of electrolyte materials is an important factor in determining the battery performance. To determine the effect of the SPB block on the electrochemical stability of the diblock copolymers, linear sweep voltammetry (LSV) measurements were carried out at 60 • C. Figure 5a shows the LSV results of PPEGMA 68 /LiTFSA and PPEGMA 68 -b-SPB 121 /LiTFSA (anodic scan from 2.9 to 5.6 V). The oxidation potential of PPEGMA was approximately 4.2 V vs. Li/Li + , which is identical to the value reported previously for PEO-based electrolytes [31]. On the other hand, the oxidation potential of PPEGMA 68 -b-SPB 121 was approximately 5.0 V vs. Li/Li + . The oxidation limit was improved from 4.2 to 5.0 V by the introduction of SPB block in the copolymer. We have already reported that the oxidation limit of oligoether electrolytes is improved from around 4.5 to over 5.0 V vs. Li/Li + by the addition of zwitterions [17,18]. The effect of zwitterion on the interfacial structures of Pt/tetraglyme (G4)-LiTFSA systems was investigated using in-situ infrared-visible sum frequency generation (IV-SFG) spectroscopy [32]. The SFG spectra confirmed that the Pt surface is covered by the Li + /zwitterion complex cations, which are more stable to oxidation than free G4 molecules. The enhancement of electro-chemical stability of PPEGMA 68 -b-SPB 121 is in good accordance with the results of G4 system, suggesting that the formation of Li + /SPB complex results in full coverage of the SPB block at the Pt electrode surface which accounts for the enhanced oxidation stability of the block copolymers.
Polymers 2021, 13, x 9 of 12 over 5.0 V vs. Li/Li + by the addition of zwitterions [17,18]. The effect of zwitterion on the interfacial structures of Pt/tetraglyme (G4)-LiTFSA systems was investigated using in-situ infrared-visible sum frequency generation (IV-SFG) spectroscopy [32]. The SFG spectra confirmed that the Pt surface is covered by the Li + /zwitterion complex cations, which are more stable to oxidation than free G4 molecules. The enhancement of electrochemical stability of PPEGMA68-b-SPB121 is in good accordance with the results of G4 system, suggesting that the formation of Li + /SPB complex results in full coverage of the SPB block at the Pt electrode surface which accounts for the enhanced oxidation stability of the block copolymers.  Figure 5b shows the CV results of PPEGMA68-b-SPB121/LiTFSA composites on Ni electrodes at 60 °C. Continuous anodic current and two reduction peaks at 0.5 and 0.8 V vs. Li/Li + were observed only at the 1st anodic scan. These anodic current and reduction peaks will be associated with the reactions of oxides and water remaining on electrode suface [33]. The voltammograms of the composite electrolyte showed a reduction peak at −0.2 V vs. Li/Li + and an oxidation peak at 0.1 V vs. Li/Li + for Li at the 1st cycle. These reduction and oxidation peaks were observed over 30 cycles. However, the current density of the peaks decreased with increasing the number of cycles. In addition, the maximum current density of the oxidation peak shifted to a higher potential value and was broadened with an increasing number of cycles. These observations has been attributed to the formation of a suitable solid electrolyte interphase (SEI) film on the electrode surface [34]. The stable stripping/plating reactions were observed over 30 cycles, indicating that the block copolymers composed of PEGMA and SPB function as a Li-ion conductor. Pristine cathode was also used for comparison. The discharge capacity of the cell employing the pristine cathode was 140 mAh g −1 during the first 10 cycles and gradually decreased with an increasing number of cycles. Finally, the cell exhibited no discharge capacity at the 50th cycle. The coulombic efficiency of the cell employing the pristine cathode exhibited the same tendency with the discharge capacity and was maintained at 95% during the first 10 cycles. The coulombic efficiency decreased with increasing cycle number and reached 0 % at the 50th cycle. On the other hand, the discharge capacity of the cell employing the cathode coated with PPEGMA68-b-SPB121 exhibited a constant value of 145  Li/Li + were observed only at the 1st anodic scan. These anodic current and reduction peaks will be associated with the reactions of oxides and water remaining on electrode suface [33]. The voltammograms of the composite electrolyte showed a reduction peak at −0.2 V vs. Li/Li + and an oxidation peak at 0.1 V vs. Li/Li + for Li at the 1st cycle. These reduction and oxidation peaks were observed over 30 cycles. However, the current density of the peaks decreased with increasing the number of cycles. In addition, the maximum current density of the oxidation peak shifted to a higher potential value and was broadened with an increasing number of cycles. These observations has been attributed to the formation of a suitable solid electrolyte interphase (SEI) film on the electrode surface [34]. The stable stripping/plating reactions were observed over 30 cycles, indicating that the block copolymers composed of PEGMA and SPB function as a Li-ion conductor. Pristine cathode was also used for comparison. The discharge capacity of the cell employing the pristine cathode was 140 mAh g −1 during the first 10 cycles and gradually decreased with an increasing number of cycles. Finally, the cell exhibited no discharge capacity at the 50th cycle. The coulombic efficiency of the cell employing the pristine cathode exhibited the same tendency with the discharge capacity and was maintained at 95% during the first 10 cycles. The coulombic efficiency decreased with increasing cycle number and reached 0 % at the 50th cycle. On the other hand, the discharge capacity of the cell employing the cathode coated with PPEGMA 68 -b-SPB 121 exhibited a constant value of 145 mAh g −1 during the first 10 cycles and gradually decreased with increasing cycle number, from 145 mAh g −1 to 120 mAh g −1 at the 60th cycle. The coulombic efficiency of the cell employing the cathode coated with the block copolymer exceeded 90% over 60 cycles. The discharge capacity and coulombic efficiency of the cell employing the coated cathode were much higher than those of the cell employing the pristine cathode at the 50th cycle. The coating of PPEGMA 68 -b-SPB 121 on the cathode surface was effective to lower the rate of cell capacity and coulombic efficiency fading in the cells at high cut-off voltage values. The effect of zwitterions on charge/discharge properties of Li/electrolyte/LiCoO 2 cells with oligoether and ionic liquid electrolytes has been reported in the same cut-off voltage range of 3.0-4.6 V [17,28,35]. Although the discharge capacities and coulombic efficiencies of the cells employing the electrolytes without zwitterions decreased with cycle number, the addition of zwitterions into the electrolytes was effective to stablilize the discharge capacities and coulombic efficiencies during 50 cycles. This should be based on the improvement of oxidation stability of electrolyte materials by the addition of zwitterions. In the cells employing the cathode coated by the block copolymers, the SPB block on the electrode surface also improves the oxidation stability of electrolyte materials at higher cut-off voltages. In general, the discharge capacity of cells employing cathode active materials such as NMC and LCO increases with increasing cut-off voltage value. This type of material, which prevents the decomposition of electrolyte materials at higher voltages, is intended for the development of deep discharge batteries and will open a new methodology to improve the charge/discharge properties of Li batteries. mAh g −1 during the first 10 cycles and gradually decreased with increasing cycle number, from 145 mAh g −1 to 120 mAh g −1 at the 60th cycle. The coulombic efficiency of the cell employing the cathode coated with the block copolymer exceeded 90% over 60 cycles. The discharge capacity and coulombic efficiency of the cell employing the coated cathode were much higher than those of the cell employing the pristine cathode at the 50th cycle. The coating of PPEGMA68-b-SPB121 on the cathode surface was effective to lower the rate of cell capacity and coulombic efficiency fading in the cells at high cut-off voltage values. The effect of zwitterions on charge/discharge properties of Li/electrolyte/LiCoO2 cells with oligoether and ionic liquid electrolytes has been reported in the same cut-off voltage range of 3.0-4.6 V [17,28,35]. Although the discharge capacities and coulombic efficiencies of the cells employing the electrolytes without zwitterions decreased with cycle number, the addition of zwitterions into the electrolytes was effective to stablilize the discharge capacities and coulombic efficiencies during 50 cycles. This should be based on the improvement of oxidation stability of electrolyte materials by the addition of zwitterions. In the cells employing the cathode coated by the block copolymers, the SPB block on the electrode surface also improves the oxidation stability of electrolyte materials at higher cut-off voltages. In general, the discharge capacity of cells employing cathode active materials such as NMC and LCO increases with increasing cut-off voltage value. This type of material, which prevents the decomposition of electrolyte materials at higher voltages, is intended for the development of deep discharge batteries and will open a new methodology to improve the charge/discharge properties of Li batteries.

Conclusions
The block copolymers, PPEGMA68-b-SPBm (m = 17, 31, 62, and 121), with well-controlled molecular weights were synthesized by RAFT polymerization. The Mn of PPEGMA68-b-SPBm was determined by 1 H NMR measurements to be in the range of 37,800 and 67,000 g mol −1 . All the neat diblock copolymers exhibited two distinct Tg values at around −75 and 5 °C, which are associated with PEGMA and SPB units, respectively. PPEGMA68-b-SPBm/LiTFSA composites also exhibited two distinct Tgs except for [EO]:[Li] = 6:1. PEGMA and SPB are incompatible components and tend to spontaneously form phase-separated structures. Microphase separation was observed for all the block copolymers and their LiTFSA composites in AFM observation. PPEGMA68-b-SPB121/LiTFSA composites exhibited higher ionic conductivities than those of the block copolymers with lower SPB contents.

Conclusions
The block copolymers, PPEGMA 68 -b-SPB m (m = 17, 31, 62, and 121), with wellcontrolled molecular weights were synthesized by RAFT polymerization. The M n of PPEGMA 68 -b-SPB m was determined by 1 H NMR measurements to be in the range of 37,800 and 67,000 g mol −1 . All the neat diblock copolymers exhibited two distinct T g values at around −75 and 5 • C, which are associated with PEGMA and SPB units, respectively. PPEGMA 68 -b-SPB m /LiTFSA composites also exhibited two distinct T g s except for [EO]:[Li] = 6:1. PEGMA and SPB are incompatible components and tend to spontaneously form phase-separated structures. Microphase separation was observed for all the block copolymers and their LiTFSA composites in AFM observation. PPEGMA 68 -b-SPB 121 /LiTFSA composites exhibited higher ionic conductivities than those of the block copolymers with lower SPB contents. The ionic conductivity of PPEGMA 68 -b-SPB 121 /LiTFSA composites increased with increasing LiTFSA concentration. These results would result in the enhancement of Li-salt dissociation by SPB units, which has high polarity. The oxidation potential of PPEGMA 68 -b-SPB 121 was approximately 5.0 V vs. Li/Li + . The oxidation limit was improved by the introduction of the SPB block in the PEO-based copolymers. The stable stripping/plating reactions of Li were observed over 30 cycles in CV measurements. The block copolymers were composed of PEGMA, and SPB functions as a Li-ion conductor. The Li/NMC cells were fabricated by using an NMC surface coated with PPEGMA 68b-SPB 121 . The discharge capacity and coulombic efficiency of the cells exhibited higher values at the 60th cycle as compared with those of the cells with pristine NMC in the cut-off voltage range of 3.0-4.6 V. The SPB block on the electrode surface improves the oxidation stability of electrolyte materials at higher cut-off voltages. Zwitterions function effectively as cathode-coating materials in Li batteries. This will be a new methodology to improve charge/discharge properties of not only Li batteries but also other rechargeable batteries.

Data Availability Statement:
The data presented in this study are available on request from the corresponding author.