A. S.
Shaplov
*a,
P. S.
Vlasov
ab,
M.
Armand
c,
E. I.
Lozinskaya
a,
D. O.
Ponkratov
a,
I. A.
Malyshkina
d,
F.
Vidal
e,
O. V.
Okatova
f,
G. M.
Pavlov
g,
C.
Wandrey
h,
I. A.
Godovikov
a and
Y. S.
Vygodskii
a
aA.N. Nesmeyanov Institute of Organoelement Compounds Russian Academy of Sciences (INEOS RAS), Vavilov str. 28, 119991, GSP-1, Moscow, Russia. E-mail: zipper@ineos.ac.ru; Fax: +7 499 1355085; Tel: +7 499 1359244
bDepartment of Macromolecular Chemistry, Saint-Petersburg State University, Universitetsky pr. 26, 198504, Saint-Petersburg, Russia
cLaboratoire de Réactivité et Chimie des Solides (LRCS), University de Picardie Jules Verne, UMR 6007 CNRS, 33 rue de Saint-Leu, 80039, Amiens, France
dDepartment of Physics, Moscow State University, Vorob'evy gory, 119992, Moscow, Russia
eLaboratoire de Physico-chimie des Polymères et des Interfaces (LPPI), Universite' de Cergy-Pontoise, 5 mail Gay-Lussac, 95031, Cergy-Pontoise, Cedex, France
fInstitute of Macromolecular Compounds Russian Academy of Sciences (IMC RAS), Bolshoy av. 31, Saint-Petersburg, 199004, Russia
gInstitute of Physics, Saint-Petersburg State University, Ulyanovskaya str. 1, Petrodvorets, 198504, Saint-Petersburg, Russia
hLaboratoire de Médecine Régénérative et de Pharmacobiologie (LMRP), Ecole Polytechnique Fédérale de Lausanne (EPFL), station 15, CH-1015, Lausanne, Switzerland
First published on 25th August 2011
Three novel ionic monomers having highly delocalized anions and electrochemically stable mobile cations, namely, 1-butyl-1-methylpyrrolidinium 1-[3-(methacryloyloxy)propylsulfonyl]-1-(trifluoromethane-sulfonyl)imide, 1-butyl-1-methylpyrrolidinium 1,1-dicyano-1-[(3-(methacryloyloxy)propylsulfonyl)]methanide and 1-butyl-1-methylpyrrolidinium 1-cyano-1-[(3-(methacryloyloxy)propylsulfonyl)]imide were synthesized and characterized. The structure of these monomers was designed to be a mimic of the most highly conductive bis(trifluoromethylsulfonyl)imide, tricyanomethanide and dicyanamide anions. By radical polymerization procedure a series of new anionic “polymeric ionic liquids” (PILs) were prepared. The solubility of these linear PILs, thermal stability, glass transition temperatures, molar masses and ionic conductivities were estimated. An advantage of the novel PILs was demonstrated by the comparison of their ionic conductivity at 25 °C (2.0 × 10−8 ÷ 1.6 × 10−7 S cm−1) with the unmodified poly(1-ethyl-1-methylpyrrolidinium 3-(methacryloyloxy)propane-1-sulfonate) analog. The increase in ionic conductivity is as high as three orders of magnitude and was found to depend on the size of the attached anion. The new ionic monomers were subsequently copolymerized with poly(ethylene glycol) dimethacrylate and poly(ethylene glycol) methyl ether methacrylate. The investigation of the copolymers properties revealed further improvement of the conductivity in approximately two orders of magnitude and the achievement of σ = 4.8 ÷ 6.8 × 10−6 S cm−1) at 40 °C.
More recently, interest has turned to the polymers based on ionic liquids and their potential application as a new class of polymers that combine all beneficial properties of ILs with those of classical polyelectrolytes.5–9 The use of “polymeric ionic liquids” (PILs) as advanced polymer electrolytes was suggested by Ohno.7,10 As in the case of ILs, one of the important advantage of PILs is their diverse chemical composition, structure, and hence properties, that can be readily changed by pairing any of a variety of organic cations with a wide range of either inorganic or organic anions. The final challenge for PILs is to achieve a high level of ion dissociation, eliminating ion pairs or aggregates, so that the conductivity becomes high enough; besides the transport number of the active ion should be the highest possible. To date lithium batteries demand solid polyelectrolyte membranes having ionic conductivity in the range of 10−5–10−4 S cm−1 at 25 °C.1 However, the most promising trend is the utilization of Li batteries in conjunction with other energy sources. Thus, as a part of energy system, Li batteries are allowed to work at higher temperatures than r.t. and at 25 °C can possess conductivity lower then mentioned one. Nevertheless, the general tendency is to have as high conductivity as possible.1,3,6,10
Taking into account that the privileged charge carrier in modern batteries is the cation (Li+ in particular) the required PILs or their copolymers should be of the polyanion type.6,11 To enhance the ion conductivity and the ion dissociation, the anionic species should be only weakly basic and preferably have a diffuse charge, as, for example, in bis(trifluoromethylsulfonyl)imide (TFSI),12–15PF6 or ClO4 anions.4,16 In its turn, ionic liquids with pyrrolidinium cations have emerged as one of the most promising ionic liquids for application in lithium batteries due to their better electrochemical stability with respect to the more frequently investigated imidazolium ILs.2,3 To our knowledge, till now only one example of utilization of PILs as solid separators in Li batteries has been published by group of D. Mecerreyes.17
Very recently, we reported the preparation and study of the conductive and mechanically stable polymer films based on (3-sulfopropyl) methacrylate polyanion and quaternized (aprotic) pyrrolidinium or imidazolium counter-ions.18 The conductivity of these PILs is greatly affected by the humidity and can increase up to 220 times while transferring from dry conditions to 20% relative humidity. Although the conductivity results at ambient temperature and humidity were satisfactory, the ionic conductivity in dry conditions was too low.
Another anionic PIL published by our group lately19 possessed structure shown on Scheme 1. The reported bulk ionic conductivity (6.5 × 10−4 S cm−1) was measured at ambient conditions, i.e. at ∼40% relative humidity. Originally, it was designed for actuator application and therefore contained less electrochemically stable imidazolium cation and –CH2–N–SO2CF3 anion having low stability towards metal lithium.
Scheme 1 |
The main goal of this work is to report the synthesis and investigation of new family of PILs not prone to water take-up and having highly delocalized anions in the polymer backbone and quaternized pyrrolidinium cations as mobile counterions. For the first time the ionic liquid like monomers (ILMs) with –SO2–C(CN)2 and –SO2–N–CN negatively charged groups as a mimic of the most highly conductive tricyanomethanide and dicyanamide anions have been designed and prepared.
Inherent viscosities (ηinh) were measured using an Ostwald capillary viscometer (0.05 g of polymer in 10.0 mL of solvent at 25.0 °C), while the intrinsic viscosities [η] were determined with an Ubbelohde type capillary viscometer at 25.0 °C.
The average MsD polymer molecular masses were determined at 25.0 °C in 0.25M 1-butyl-1-methylpyrrolidinium bromide ([1-Bu-1-MePyrr]Br) solution in DMF for poly-9 and poly-10 by sedimentation-diffusion analysis. The density and viscosity of the 0.25M [1-Bu-1-MePyrr]Br solution in DMF were determined as ρo = 0.9593 g cm−3 and ηo = 0.9437 cPa. Velocity sedimentation was performed in a Beckman XLI analytical ultracentrifuge (ProteomeLab XLI Protein Characterization System, Beckman Coulter Inc., USA) at a rotor speed of 40 × 103 rpm. The buoyancy factor (1 − υρ0) and the partial specific volumes υ (0.733 and 0.817 mL g−1 for poly-9 and poly-10, correspondingly) were estimated from the solution densities measured by the DMA-4000 densitometer (Anton Paar GmbH, Austria). The dn/dc values for poly-9 and poly-10 were determined as 0.039 and 0.076 g mL−1, respectively.
The glass transition temperatures (Tg) of the linear PILs were determined by thermomechanical analysis (TMA) using a UIP-70M (Russia) thermomechanical analyzer at a heating rate of 2.5 °C min−1 and a constant load of 0.08 MPa. Dynamic Mechanical Thermal Analysis (DMTA) measurements were carried out on copolymer (coPILs) films (typically length × width × thickness = 15 × 8 × 0.5 (mm)) with a Q800 model (TA Instruments, USA) operating in tension mode (strain between 0.05 and 0.07%, pretension: 10−2 N). Experiments were performed at 1 Hz frequency with a heating rate of 3 °C min−1 from −90 to +150 °C. The set up provided the storage and loss modules (E′ and E′′). The damping parameter or loss factor (tanδ) was defined as the ratio tanδ = E′′/E′. Thermogravimetric analysis (TGA) was performed in air on a Q50 model (TA Instruments, USA) applying a heating rate of 5 °C/min.
The efficiency of the cross-linking reactions between the ILMs, PEGDM and PEGM was estimated by the extraction of the copolymer films in a Soxhlet extractor with dichloromethane for 10 h with subsequent drying in a vacuum at 80 °C over night.
Dielectric spectroscopy studies of monomers, PILs and coPIL's films were run on a Novocontrol Broadband Dielectric Spectrometer equipped with an Alpha analyzer and a Quatro temperature controller (Novocontrol GmbH, Germany). The films were preliminarily dried in a vacuum oven containing a Petri dish with P2O5 at 80 °C/1 mm Hg and then sandwiched between the gold-coated brass electrodes. The experiments were carried out at 25 °C in the 10−1–107 Hz frequency range in air. Conductivities were duplicated by complex impedance analysis using impedance analyzer Autolab PGSTAT30 (Autolab Frequency Response Analyser System, Metrohm Autolab B.V., The Netherlands). The runs were performed in air, varying the frequency from 10−2 to 108 Hz at 25 °C. A polymer film was put in a cell with pressure contact stainless steel electrodes.
Scheme 2 Synthetic route for the preparation of monomers 9, 10 and 11. Reagents and conditions: (i) SOCl2, THF/DMF, 0 °C → RT; (iia) NH2SO2CF3, THF, NEt3, 0 °C → RT; (iib) CH2(CN)2, THF, NEt3, 0 °C → RT; (iic) NH2CN, THF, NEt3, 0 °C → RT; (iii) LiH, THF, 10 °C → RT; (iv) 1.4 [1-Bu-1-Me Pyrr]Br, H2O, RT. |
For the preparation of monomers 9–11 the synthetic method consisting of four steps (Scheme 2) was developed. On the first stage potassium 3-(methacryloyloxy)propane-1-sulfonate was converted into the sulfonyl chloride derivative by reaction with thionyl chloride in the presence of DMF as a catalyst. This reaction can be carried with/without anhydrous THF as a co solvent. The presence of THF as a solvent was influencing only the yield of the reaction, i.e. slightly increasing it to 80%. Due to the hydrophobic nature of 2 as well as its relative stability towards cold water in comparison with carboxylic acid chlorides,22 it was isolated from the reaction mixture by pouring into the ice-water. The subsequent extraction with methylene chloride and drying over magnesium sulfate resulted in the obtaining of 2 in high purity.
The second stage consisted in the reaction of 2 with trifluoromethanesulfonamide (Scheme 2, 3), malononitrile (Scheme 2, 4) or cyanamide (Scheme 2, 5) in the presence of a 2.2 molar excess of triethylamine. When the reaction was carried out in 1:1 molar ratio between the 2 and triethylamine, the triethylammonium hydrochloride was isolated only in 50% yield and the inseparable mixture of 3 and its acid form (in 1:1 ratio according to NMR) was obtained. Thus, it was found that the desired monomeric acids can be successfully isolated only in the form of their triethylammonium salts (Scheme 2, 3, 4 or 5). Further studies revealed that triethylamine appeared to be the best reagent for this reaction. Its substitution with pyridine, a weaker base, did not result in the isolation of the target compound. According to22,23 the similar reaction of aliphatic sulfonyl halides with nucleophiles proceeds via one of the two competing pathways: nucleophilic substitution (nucleophilic reaction and general-base mechanism) or elimination-addition mechanism (formation of sulfenes R–CH = SO2). The realization of the specific mechanism was found to be dependent on the reaction conditions including the nature of the base.23 As far as the nitrogen atom in triethylamine is less nucleophilic and more hindered than in pyridine, the sulfene mechanism may predominate. The application of stronger bases, such as NaH and EtONa, was complicated by various side reactions of cyano groups and resulted in intensively colored and insoluble products. The third stage of the suggested synthetic path was concluded in the interaction of 3–5 with lithium hydride in anhydrous THF (Scheme 2). To exclude the possibility of an ionic polymerization, the reaction was started at temperatures < −10 °C. However, probably due to the limited solubility of LiH in the anhydrous THF, this reaction proceeded smoothly only at 10 °C, that was monitored by the visible evolution of hydrogen. After the removal of the excess of lithium hydride by filtration, 6–8 were recovered as highly viscous colored oils in a virtually quantitative yield. It was further revealed that 6 and 8 can be additionally recrystallized from anhydrous methylene chloride as white needle like crystals.
The final step represented a metathesis reaction between the lithium salts of the desired monomers (Scheme 2, 6, 7 and 8) and the respective pyrrolidinium bromide ionic liquid. As in the synthesis of bis(trifluoromethylsulfonyl)imide containing ILs,24 the reaction leads to the preparation of clean products. The hydrophobic 9 and 10 precipitated from the aqueous medium and can be easily isolated. In contrast, the cyanamide derivative 11 appeared to be somewhat hydrophilic and water miscible. However, it was possible to extract it with methylene chloride and recover after the solvent evaporation in 78% yield. It should be noted that monomers 9–11 after their isolation need to be stored at low temperatures in the presence of dissolved 4-methoxyphenol (inhibitor).
The structure and purity of 9–11 were proved by 1H and 13C NMR, IR spectroscopy and elemental analysis. All three ILMs represent viscous liquids at r.t. To study their thermal behavior the differential scanning calorimetry (DSC) was used. The DSC traces performed with a slow rate of 2 °C min−1 confirmed the absence of any crystallization or melting processes for the studied ionic compounds. The monomers showed only glass transition Tg at −71.0, −69.9 and −75.5 °C for 9, 10 and 11, respectively. As expected, ionic monomer 11 having the smallest delocalized anion with little rotational barrier of S–N bond demonstrates the lowest Tg.
The ionic conductivity measured for cited monomers resulted in the values of 1.4 − 3.1 × 10−4 S cm−1 at 25 °C. In spite of the difference in the nature of the attached anion, 9–11 visibly seemed to have similar viscosity and as a result demonstrated nearly equal conductivity. Evidently the large size of the anionic part imparts high viscosity for the investigated ILMs, that in its turn reduces the ion mobility and the ionic conductivity in comparison with the analogous 1-butyl-1-methylpyrrolidinium bis(trifluoromethylsulfonyl)imide ionic liquid (σ = 2.2 × 10−3 S cm−1).14
No | Polymer | η inh (dL g−1)a | [η] (dL g−1)b | MsD (g mol−1)c | Tg (°C)d | σDC (S cm−1) e | T d (°C)f | |
---|---|---|---|---|---|---|---|---|
a For the solution of 0.05 g of polymer in 10.0 mL of DMF at 25.0 °C. b For the solution of polymer in 0.25 M [1-Bu-1-MePyrr]Br in DMF at 25.0 °C. c Determined by sedimentation-diffusion analysis in 0.25M [1-Bu-1-MePyrr]Br in DMF. d Tg was determined by TMA. e Conductivity of polymer film at 25 °C. f Onset loss temperature according to TGA. | ||||||||
1 | poly-9 | 3.17 | 0.77 | 0.5 × 106 | 14 | 2.0 × 10−8 | 285 | |
2 | poly-10 | 5.29 | 2.00 | 1.7 × 106 | 38 | 3.1 × 10−8 | 235 | |
3 | poly-11 | 3.20 | 0.71 | — | 11 | 1.6 × 10−7 | 245 |
The determination of [η] in DMF was complicated by the insufficient electrostatic screening. To suppress it, 1-butyl-1-methylpyrrolidinium bromide was added to DMF. The addition of pyrrolidinium based IL instead of standard salt electrolyte (LiCl, Li(CF3SO2)2N, etc.) was driven by the aim to exclude the ion exchange between the mobile pyrrolidinium cation of the polyelectrolyte and the metal ions. The use of 0.25 M solution of 1-butyl-1-methylpyrrolidinium bromide in DMF as a solvent yielded the intrinsic viscosities 0.77, 2.00 and 0.71 dL g−1 for poly-9, poly-10 and poly-11, respectively (Table 1).
The sedimentation-diffusion analysis was applied for investigation of poly-9 and poly-10 molar masses (Table 1). 0.25 M solution of 1-butyl-1-methylpyrrolidinium bromide in DMF was used as a solvent for the study of the sedimentation velocity and the translational diffusion. The molar mass (MsD) determined by this method was equal to 500 × 103 and 1700 × 103 g mol−1 for poly-9 and poly-10, respectively.
In spite of the apparent similarity of monomer structures, the solubility of poly-9–poly-11 are different (Table 2). The most pronounced disparity concluded in the hydrophobic nature of poly-9 and poly-10 and hydrophilicity of poly-11, soluble in water and aq. 0.5 M NaCl. While in DMF all three studied polymers were soluble, DMSO was capable to dissolve only poly-9 and poly-10. Poly-9 and poly-10 were soluble in tetrachloroethane/phenol mixture. The solubility of poly-9 in acetone and poly-10 in methanol deserves to be noted. In contrast to the majority of hydrophobic PILs, the solubility of poly-10 in methanol was found to be its distinctive peculiarity. At the same time the uncommon solubility of poly-9 in acetone can be attributed to the fluorinated nature of the attached anion. As well as ILs, poly-9–poly-11 were soluble in acetonitrile and insoluble in diethyl ether.
Solvent | Polymer | ||
---|---|---|---|
poly-9 | poly-10 | poly-11 | |
a Solubility: (+) soluble at ambient temperature, (+t) soluble on heating, (±) partly soluble on heating, (–) insoluble even on heating. | |||
DMF | + | + | + |
0.5 M Li(CF3SO2)2N in DMF | + | + | — |
DMSO | + | + | — |
H2O | — | — | +t |
0.5 M NaCl in H2O | — | — | +t |
Methanol | — | + | — |
HFIP | ± | ± | ± |
Acetone | + | — | — |
Acetonitrile | + | + | + |
CH2Cl2 | — | — | — |
Chloroform | — | — | — |
Cyclohexanone | — | — | — |
Diethyl ether | — | — | — |
Symm-Tetrachloroethane/phenol (3:1, by wt) | + | + | ± |
Thermal stability of novel PILs (onset temperature of polymer degradation, Td) and their heat resistance (Tg) were estimated (Table 1). Poly-9 demonstrated the highest Td among the investigated polymers. The thermal stability of poly-10 and poly-11 was lower by 40–50 °C and equal to 235 and 245 °C, respectively. Tgs of poly-9 and poly-11 are in the order: poly-11 < poly-9 < rt < poly-10 (Table 1). Upon consideration of poly-9–poly-11 as polymeric analogs of 1-butyl-1-methylpyrrolidinium bis(trifluoromethylsulfonyl)imide, tricyanomethanide and dicyanamide ILs, respectively, it was of interest to compare their thermal properties. It is of common knowledge, that bis(trifluoromethylsulfonyl)amide anion usually imparts high thermal stability to the respective ILs, increasing their Td over 420 °C.4 The thermal decomposition temperatures for the tricyanomethanide ILs vary between 290 and 335 °C25 that are quite similar to the dicyanamide salts.26 According to the onset temperature of decomposition ILs follow the general stability order: [1-Bu-1-MePyrr]N(CF3SO2)2 > [1-Bu-1-MePyrr]C(CN)3 ≥ [1-Bu-1-MePyrr]N(CN)2. It is noteworthy, although the thermal stability of poly-9–poly-11 is lower in comparison with the corresponding ILs, their thermal properties (both Td and Tg) follow the same general tendencies.
According to the values of ionic conductivity at 25 °C the investigated polyelectrolytes can be arranged in the following order: poly-11 > poly-10 > poly-9 (Table 1). Such sequence is in a full agreement with the conductivity of the ILs with dicyanamide, tricyanomethanide and bis(trifluoromethylsulfonyl)imide mobile anions.3,27 The higher conductivity of poly-11 can be attributed to the smallest size of the –SO2–N–CN anion.
A clear advantage of the achievement of high delocalization in the attached anion can be demonstrated by comparison of poly-9–poly-11 and unmodified poly(1-ethyl-1-methylpyrrolidinium 3-(methacryloyloxy)propane-1-sulfonate) (Scheme 3, poly-12). The ionic conductivity of poly-9–poly-11 at 25 °C (2.0 × 10−8 ÷ 1.6 × 10−7 S cm−1) was found to be two or three orders of magnitude higher than that of poly-12 (3.3 × 10−10 S cm−118). At the same time Tg of poly-9–poly-11 (11 ÷ 38 °C) were close to r.t. and lower than the Tg of poly-12 (63 °C18). Thus, PILs containing weakly nucleophilic attached anions are more conductive and demonstrate lower Tgs. Another interesting comparison can be performed on poly-9 and structurally similar poly-13 (Scheme 3). The latter polycation serves as a good reference as it has the same polymer backbone and the same length of the alkyl spacer. Tg of poly-13 is higher (55 °C18) while its conductivity (7.8 × 10−9 S cm−116) is lower in comparison with anionic poly-9. Probably, at similar degree of delocalization of the imide anions in polycation and polyanion, the presence of mobile bulky 1-butyl-1-methylpyrrolidinium cation in poly-9 leads to the loosening of the polymer packing and subsequent decrease of the polymerTg and an increase in ions mobility.
Scheme 3 Chemical structures of poly-9, unmodified poly-12 and structurally similar polycation poly-13. |
No | Composition | T α (°C)a | σDC, (S cm−1)b | T d (°C)c | ||
---|---|---|---|---|---|---|
ILM | PEGDM (wt%) | PEGM (wt%) | ||||
a T α was determined by DMTA. b Conductivity of polymer film at 25 °C. c Onset loss temperature according to TGA. | ||||||
1 | 30 | — | 5.5 | 5.5 × 10−7 | 230 | |
2 | 20 | 10 | −1.4 | 2.0 × 10−6 | 215 | |
3 | 30 | — | 15.0 | 6.7 × 10−7 | 230 | |
4 | 20 | 10 | 0.6 | 2.7 × 10−6 | 230 | |
5 | 30 | — | 4.4 | 2.9 × 10−7 | 230 | |
6 | 20 | 10 | −2.1 | 1.5 × 10−6 | 215 |
Fig. 1 DMTA analysis for PEGDM film (11) and copolymer films: coPEGDM/PEGM (22), copoly-9/PEGDM (33) and copoly-9/PEGDM/PEGM (44). |
The copolymerization of the 9–11 was further performed with both PEGDM and PEGM (Table 3, entries 2, 4 and 6). The tercopolymerization resulted in the next decrease of the Tg to the region close to or less than 0 °C. In turn, the simultaneous reduction of the Tg and the increase of the degrees of freedom (“dangling chains” effect1) led to the significant increase of the bulk ionic conductivity. It is noticeable that all three copolymer films demonstrated at 25 °C practically equal conductivity which moved to the 10−6 S cm−1 region (Table 3, entries 2, 4 and 6).
To check the copolymerization reaction completion and the presence of any unpolymerized ionic monomers or oligomers which can influence PIL's properties, the obtained films were extracted with CH2Cl2. It was found that the soluble fraction content is quite low (0.8–4.2 wt%) which proves the high efficiency of the cross-linking reaction. Additionally, the tan δ vs. temperature dependence for all obtained copolymers showed single narrow relaxation peaks (Fig. 1).
Fig. 2 shows the temperature dependence of the ionic conductivity for tercopolymers of 9 and 10. The observed dependence was found to be nonlinear. However, in accordance with the general tendency, the ionic conductivity rises significantly with temperature. Thus, at 40 °C the σ values were two times higher than at r.t. and were equal to 4.8 × 10−6 and 6.8 × 10−6 S cm−1 for poly-9/PEGDM/PEGM and poly-10/PEGDM/PEGM, respectively. Reaching 10−5 S cm−1 was observed already at 45–48 °C.
Fig. 2 Temperature dependence of ionic conductivity for copoly-9/PEGDM/PEGM (11) and copoly-10/PEGDM/PEGM (22) films. |
TGA of the obtained copolymers revealed almost identical (∼230 °C) onset loss temperature (Table 3). This can be explained by the fact that the thermal stability of these films is mainly governed now by the decomposition of the PEO fragments.
The subsequent copolymerization of ILMs with PEGDM and PEGM leads to the preparation of novel solid polymer electrolytes with enhanced ionic conductivity. The conductivity of polymer films achieved at 40 °C was 4.8÷6.8 × 10−6 S cm−1, while already at 45–48 °C, σ reached 10−5 S cm−1. These findings along with polymer good thermal stability make them attractive candidates for the application as materials in various electrochemical devices.
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