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Page 4 of 12               Cui et al. Energy Mater 2023;3:300034  https://dx.doi.org/10.20517/energymater.2023.19

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               approximately 2,300 cm , which indicates that isocyanate has been completely consumed by the
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               polyaddition reaction. The existence of C-SO -N bonds (1,195 cm ) and C-S bonds (1,061 cm ) is
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               associated with LiTFSI. The existence of the -CH - component (2,918 cm ) and C-O-C bonds (1,135 cm ) is
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               assigned to PU segments. We also recorded FTIR spectra of the PO membrane and PU-LITFSI (PO-PU-
               LITFSI electrolyte without PO membrane). After adding the PO skeleton to PU-LiTFSI, the peak positions
               of PU-LiTFSI did not shift and no additional peaks were observed, indicating that the PO skeleton does not
               react with other components and exists stably in the PO-PU-LiTFSI electrolyte [Supplementary Figure 1].
               Furthermore,  TGA  reveals  that  the  PO  and  PU  contents  were  5  wt%  and  15  wt%,  respectively
               [Supplementary Figure 2] .
                                     [23]
               The  PO-PU-LiTFSI  electrolyte  shows  high  mechanical  strength.  As  shown  in  Figure 2 A  and
               Supplementary Figure 3, the puncture resistance of the PO-PU-LiTFSI electrolyte is as high as 4.6 N, and its
               tensile strength is 145.1 MPa. The tensile strength of the PO-PU-LiTFSI electrolyte is one of the best
               performances among reported SPE [Supplementary Table 1]. The high strength of the electrolyte is related
               to the high strength of the PO membrane. The puncture resistance and tensile strength of the PO-PU-
               LiTFSI electrolyte are about 10% higher than those of the PO membrane, which indicates that PU-LiTFSI
               modification can improve the strength of the PO skeleton.


               The PO-PU-LiTFSI electrolyte exhibits high adhesion. The adhesive force between the PO-PU-LiTFSI
               electrolyte and S cathode is 4.15 N, and the value between the electrolyte and Li anode is 2.36 N [Figure 2B
               and Supplementary Figure 4A]. The high adhesion is related to high mobility of PU segments and the
               strong interactions (such as H-bonding) between urethane/urea groups and other polar groups . The high
                                                                                               [24]
               mobility of PU segments was reflected by the differential scanning calorimetry (DSC) curves and X-ray
               diffraction (XRD) patterns. As shown in the DSC curves [Figure 2C], the peak at approximately -35 °C
               corresponds to the glass transition temperature (T ) of the amorphous PU segments and the peak at
                                                             g
                                                                                               [23]
               approximately 45 °C corresponds to the melting point (T ) of the crystalline PU segments . The DSC
                                                                  m
               curve of the PU-LiTFSI (LiTFSI: 80 wt%) shows no obvious peak at approximately 45 °C, indicating that the
               PU segments in the electrolyte are amorphous. Meanwhile, no sharp diffraction peaks are detected at the
               XRD pattern [Supplementary Figure 5], which also indicates the low crystallinity of PU segments.

               The high mobility of PU segments is associated with the plasticizing effect of dissociated LiTFSI in the PO-
               PU-LiTFSI electrolyte [Figure 3A]. The plasticizing effect enhances with increasing LiTFSI content
               [Supplementary Figure 4B]. In contrast, LiTFSI in the PO-PEO-LiTFSI electrolyte cannot be dissociated at a
               high content. Therefore, the PEO segments in the PO-PEO-LiTFSI electrolyte exhibit poor mobility,
               resulting in poor contact with electrode [Figure 2B and C, Supplementary Figures 4A and 6]. The high
               LiTFSI dissociation in the PO-PU-LiTFSI electrolyte is related to a strong interaction between
               urethane/urea groups and TFSI . Density functional theory (DFT) calculations indicate that the binding
                                          -
               energies (E ) between the urethane/urea group and TFSI  are 0.76 eV, respectively, which is higher than the
                                                               -
                        ads
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               values between ether oxygen of PEO and TFSI  [Figure 3B]. The high binding energy can promote the
               dissociation of LiTFSI [25,26] . The interaction between urethane/urea groups and TFSI  was also reflected by
                                                                                       -
               the FTIR spectra of PU and PU-LiTFSI [Supplementary Figure 6]. After adding LiTFSI to PU, the N-H peak
               of PU shifted from 3,543 to 3,560 cm , while the C-N peak shifted from 1,360 to 1,348 cm . In addition, the
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               C-O-C peak shifted from 1,107 to 1,135 cm . These peak shifts indicated the interaction between urethane/
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               urea groups and TFSI . -
               The PO-PU-LiTFSI electrolyte exhibits high ionic conduction. The room-temperature ionic conductivity
                                    +
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                         -4
                                                                                  +
               (σ = 1.8 × 10  S cm ), Li   t r a n s f e r e n c e   n u m b e r   ( t   =   0 . 5 4 )   a n d   Li   d i f f u s i o n   c o e f f i c i e n t
                                                                +
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