Polymer–Ceramic Framework Stabilized Solid Electrolyte for Advanced Lithium-Ion Energy Storage

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Abstract Advancing lithium-metal solid-state batteries (LSSBs) demands innovative composite solid electrolytes with superior safety, energy density, and cycle life. Here, we report a high-performance polymer-ceramic composite solid electrolyte (PCCSE) engineered by integrating lithium perborate (LiBO 3 ) and surface-functionalized lithium lanthanum zirconium oxide (LLZO) nanofibers into a polyethylene oxide/polyvinylidene fluoride (PEO/PVDF) matrix using an optimized Stokes’ solution casting method. The synergistic interplay of LiBO 3 and LLZO disrupts polymer crystallinity, enhances amorphization, and facilitates ionic transport through robust polymer–ceramic interfacial interactions. Advanced characterization via X-ray diffraction (XRD), Fourier-transform infrared spectroscopy (FTIR), ultraviolet–visible spectroscopy (UV–Vis), and electrochemical impedance spectroscopy (EIS) confirms reduced crystallinity, improved segmental chain mobility, and optimized ionic pathways. The resulting PCCSE achieves a remarkable ionic conductivity of 4.25 × 10 − 5 S cm -1 at room temperature and a wide electrochemical stability window of 5.33 V, enabling compatibility with high-voltage cathodes. Full-cell tests with a lithium metal anode and LiCoO₂ cathode demonstrate high specific capacity, exceptional rate capability, and 95% capacity retention after 100 cycles. The PCCSE effectively mitigates lithium dendrite growth through uniform ion conduction and enhanced interfacial stability. These findings position PCCSE as a promising, safe, and high-performance electrolyte for next-generation all-solid-state lithium-metal batteries, paving the way for scalable, high-energy-density energy storage solutions.
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Here, we report a high-performance polymer-ceramic composite solid electrolyte (PCCSE) engineered by integrating lithium perborate (LiBO 3 ) and surface-functionalized lithium lanthanum zirconium oxide (LLZO) nanofibers into a polyethylene oxide/polyvinylidene fluoride (PEO/PVDF) matrix using an optimized Stokes’ solution casting method. The synergistic interplay of LiBO 3 and LLZO disrupts polymer crystallinity, enhances amorphization, and facilitates ionic transport through robust polymer–ceramic interfacial interactions. Advanced characterization via X-ray diffraction (XRD), Fourier-transform infrared spectroscopy (FTIR), ultraviolet–visible spectroscopy (UV–Vis), and electrochemical impedance spectroscopy (EIS) confirms reduced crystallinity, improved segmental chain mobility, and optimized ionic pathways. The resulting PCCSE achieves a remarkable ionic conductivity of 4.25 × 10 − 5 S cm -1 at room temperature and a wide electrochemical stability window of 5.33 V, enabling compatibility with high-voltage cathodes. Full-cell tests with a lithium metal anode and LiCoO₂ cathode demonstrate high specific capacity, exceptional rate capability, and 95% capacity retention after 100 cycles. The PCCSE effectively mitigates lithium dendrite growth through uniform ion conduction and enhanced interfacial stability. These findings position PCCSE as a promising, safe, and high-performance electrolyte for next-generation all-solid-state lithium-metal batteries, paving the way for scalable, high-energy-density energy storage solutions. Lithium-metal solid-state battery Polymer blend matrix Polymer composite ceramflux solid electrolyte LLZO Ceramic Fillers Figures Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 6 Figure 7 Figure 8 Figure 9 Introduction Lithium-metal batteries (LMBs) are pivotal to modern energy storage, powering portable electronics with their high energy density, specific capacity, and extended cycle life. However, the surging demand for ultra-high-energy-density batteries, driven by the proliferation of smart devices and large-scale applications such as electric vehicles and grid storage, has intensified safety concerns (Ding et al. 2019 ). These stem primarily from the volatility of organic liquid electrolytes, which pose risks of leakage and flammability, and the challenges associated with transitioning from graphite to lithium-metal anodes, notably lithium dendrite growth, which compromises battery safety and performance (Liu et al. 2011 ). To address these issues, lithium-metal solid-state batteries (LSSBs) have emerged as a transformative solution, replacing liquid electrolytes with solid-state alternatives (Han et al. 2020 ). LSSBs offer compelling advantages, including enhanced safety, wider electrochemical stability windows, broader operating temperature ranges, and the potential for compact, direct-stacking architectures, positioning them as a cornerstone for next-generation energy storage (Lee et al. 2022 , Li et al. 2021 ). Among solid electrolyte materials, polyethylene oxide (PEO)-based polymers have garnered significant interest due to their ability to form stable Li-salt complexes that facilitate ion transport (D’Epifanio et al. 2004 ). However, their semi-crystalline nature at room temperature limits ionic conductivity by restricting segmental chain mobility, while their modest mechanical strength fails to suppress lithium dendrite growth during cycling (Kannadasan et al. 2024 , Wang et al. 2005 ). To overcome these limitations, blending PEO with polyvinylidene fluoride (PVDF) to form a polymer blend matrix (PBM) has proven effective (Nasir et al. 2007 , Xi et al. 2006 ). PVDF contributes high mechanical strength, electrochemical stability, and favorable interactions with lithium salts, enhancing the thermal stability and amorphous content of the PEO-PVDF blend (Li et al. 2025 , Wu et al. 2021 ). This synergy improves ionic conductivity and electrode-electrolyte interfacial compatibility, yet achieving optimal ionic conductivity and dendrite suppression at ambient conditions remains a critical challenge. To further enhance performance, lithium perborate (LiBO 3 ), a dimeric salt with water of hydration (Li 2 [B 2 (O 2 ) 2 (OH) 4 ]·4H 2 O), has been incorporated as a cost-effective, environmentally benign, non-toxic lithium salt and its gives hydrogen peroxide on hydration (Pandurangan et al. 2024 , Li et al. 2024 ). LiBO 3 increases the concentration of mobile lithium ions, disrupts ion pairing within the PBM, and reduces PEO crystallinity, thereby boosting ionic conductivity and electrochemical stability (Sampathkumar et al. 2019 ). Its compatibility with PEO-PVDF blends further enhances miscibility and widens the operating voltage window, offering a sustainable alternative to conventional salts like LiClO 4 , LiTFSI, and LiBF 4 . To address mechanical and ionic conductivity limitations, lithium lanthanum zirconium oxide (LLZO), a garnet-structured ceramic, is integrated as a filler (Hegazy et al. 2022 , Hu et al. 2022 ). LLZO’s high ionic conductivity, exceptional mechanical strength, and stability against lithium metal provide additional ion conduction pathways, reduce polymer crystallinity, and effectively suppress dendrite growth. The synergistic combination of PEO, PVDF, LiBO 3 , and LLZO yields a polymer composite ceramflux solid electrolyte (PCCSE), which combines the flexibility and interfacial compatibility of the PBM, the enhanced conductivity and stability of LiBO 3 , and the mechanical and ionic transport benefits of LLZO. This study presents the synthesis and characterization of a novel PCCSE comprising PEO/PVDF, LiBO 3 , and LLZO, tailored for LSSBs with a lithium-metal anode and a lithium cobalt oxide (LiCoO 2 ) cathode (Li et al. 2021 ). Emphasis is placed on elucidating the interfacial interactions among the PBM, LiBO 3 , and LLZO, which critically govern ion transport, mechanical properties, and electrochemical performance. By addressing the longstanding challenges of ionic conductivity, mechanical stability, and dendrite suppression, this PCCSE represents a significant advancement in LSSB technology, with far-reaching implications for electric vehicles, grid-scale energy storage, and the future of sustainable energy systems. Experimental Section Materials A combination of different chemicals was used to prepare the PCCSE material, such as Lithium carbonate (Li 2 CO 3 , from Sigma-Aldrich), Lanthanum oxide (La 2 O 3 , from Alfa Aesar), Ethylene glycol (C 2 H 6 O 2 , from Merck), Zirconium ethoxide (Zr(OC 2 H 5 ) 4 , from Alfa Aesar), Dilute Nitric acid (HNO 3 , from Sigma-Aldrich), Citric acid (C 6 H 8 O 7 , from Sigma-Aldrich), Ethanol (C 2 H 5 OH, from Merck), Polyethylene oxide (PEO) from Merck, Polyvinylidene fluoride (PVDF, from Merck),), Dimethylformamide (DMF, from Merck), Lithium perborate tetrahydrate (LiBO 3 .4H 2 O, from Alfa Aesar). Only analytically pure, high-quality compounds were employed in this study (Patla et al. 2018 ). Preparation of LiLaZrO (LLZO) powder A mixture of Li 2 CO 3 , La 2 O 3 , Zr(OC 2 H 5 ) 4 , C 6 H 8 O 7 (as an organic complexing agent), and C 2 H 6 O 2 (as an organic medium) was prepared at a molar proportion of 7:3:4:28:14 as the reactant material. La 2 O 3 and Li 2 CO 3 were solubilised in HNO 3 , whereas Zr(OC 2 H 5 ) 4 was dissolved in pure C 2 H 5 OH. The two liquid phases were then combined, and C 6 H 8 O 7 and C 2 H 6 O 2 subsequently incorporated into the formulation. The resulting mixture solution was vigorously stirred and heated at 70°C to evaporate the solvent. The synthesized sol was subsequently left to dry at 110°C for 12 hours. Upon drying, the gel obtained was subjected to heat at 600°C over 120 minutes periods, later on sintering at 800° C for 600 minutes to yield Li 7 La 3 Zr 2 O 12 powder (Sakamoto et al. 2013 ). Preparation of PEO/PVDF-LiBO-LLZO A Stokes' solution-casting method was adopted to prepare PCCSE. Solutions of the PEO/PVDF PBM with a compositional mass ratio of 80/20 wt% were prepared by dissolving PEO (800 mg) and PVDF (200 mg) in conical glass flasks with stopper, followed by dissolving them in 15 ml of DMF at 80°C with constant stirring using magnetic stirrer. Thereafter, 30 wt% of LiBO 3 (0.30 g) in relation to the polymer blend, it was incorporated, followed by magnetic stirring to completely solvate the salt, resulting in polymeric blend matrix electrolyte ((80PEO/20PVDF)/30 wt% LiBO 3 ). The required amount of LLZO (0.05 g), corresponding to 5 wt% with respect to the polymeric blend matrix electrolyte (1 g), was mixed in DMF and then combined with the polymeric blend matrix electrolyte solutions. The mixture was then cast onto Teflon-coated plates and placed on a heating plate at 75°C, allowing the solvent to evaporate completely. The films were then cooled to room temperature, then subjected to vacuum drying at 40°C for a day to remove any residual solvent, and stored in desiccators (Dhatarwal and Sengwa 2019 ). Characterization Physical characteristics The crystal structures of the PEO, PVDF, PEO/PVDF, LiBO 3 , LLZO and PEO/PVDF-LiBO 3 -LLZO electrolytes were investigated using XRD analysis with a Rigaku RU-200B diffractometer and Cu Kα radiation (λ = 1.5406 Å). XRD measurements, taken at 5°C/min scanning speed and 40 an operating voltage, covering a 2θ range of 10–90°, revealing the crystalline phases. Differential scanning calorimetry (DSC) using a DSC 7 Perkin Elmer instrument elucidated the thermal behaviour and LiBO 3 solid electrolyte, and LLZO filler. (Tamaño-Machiavello et al. 2015 ) DSC analysis provided insights into the phase transitions, melting points, and crystallization behaviour, highlighting influence the LLZO filler on the properties. FTIR by employing a Thermo Nicolet 380 spectrometer was used to analyze the molecular structure by measuring the infrared radiation absorption. A Cary 60 UV–Vis spectrophotometer (Agilent, USA) was used for absorption analysis over the wavelength range of 200 − 1000 nm. The band gap of the electrolytes are calculated using $$\:E=\:\frac{1240}{\lambda\:}$$ Where, E = Band gap in eV 𝛌 = wavelength in nm 1240 is the wavelength incident on 1eV (López and Gómez 2011 ). Chemical characteristic LSV was used to examine the electrochemical behaviour and redox reaction kinetics by sweeping the working electrode potential linearly with time using an electrochemical analyzer (CHI-6650; CH Instruments) at 60 o C at a rate of 1.0mVs − 1 between the range of 2 and 6 V. Electrochemical impedance spectroscopy (EIS) provides insights into electrode-electrolyte interfaces and charge transfer processes using a small amplitude AC potential (Rathika et al. 2017 ). Charge-discharge test and galvanostatic cycling tests were used to evaluate the electrochemical performance and cycling stability through repeated charging and discharging at controlled current densities. LSSBs batteries are fabricated with a lithium metal anode, lithium cobalt oxide (LiCoO 2 ) cathode and prepared PCCSE (Li et al. 2021 ). Schematic illustration of a lithium-metal solid-state battery A schematic illustration of a lithium-metal solid-state battery is shown in Fig. 1 . The battery features a Li metal anode and lithium cobalt oxide (LiCoO 2 ) cathode, with a polymer composite ceramflux solid electrolyte (PCCSE) in between. The PCCSE consists of a polymer blend matrix composed of polyethylene oxide (PEO) and polyvinylidene fluoride (PVDF), providing a flexible and process able medium for lithium-ion transport. Embedded within this matrix are lithium perborate (LiBO 3 ), an environmentally friendly, cost-effective, and non-toxic solid electrolyte known for its mild oxidizing properties and wide applicability, and lithium lanthanum zirconium oxide (LLZO), a ceramic filler that significantly enhances ionic transport and thermal resistance. This configuration leverages the processability and flexibility of the PBM in conjunction with the high ion conductivity and thermal stability of ceramic materials, resulting in improved overall performance, safety, and longevity of the battery. Result and discussion Physical characteristics Fig. 2 shows the XRD patterns of PEO, PVDF, PEO/PVDF blend, LiBO 3 , LLZO, and the PEO/PVDF-LiBO 3 -LLZO (PCCSE) (Jacob 1997). PEO exhibits characteristic sharp peaks at 19.2° and 23.6° (2θ), confirming its semicrystalline nature, while PVDF shows distinct crystalline reflections at 18.3°, 20.5°, and 26° (2θ). The PEO/PVDF blend demonstrates reduced peak intensities compared to the individual polymers, indicating a suppression of PEO crystallinity due to intermolecular interactions between the two polymers. Upon the incorporation of LiBO 3 electrolyte and LLZO fillers into the PEO-PVDF matrix, the PCCSE shows further reduction in crystallinity, along with new diffraction peaks corresponding to the ceramic phases. These results confirm that the PEO/PVDF-LiBO 3 -LLZO composite effectively suppresses crystallinity and promotes phase integration, suggesting strong polymer-ceramic interactions that enhance its performance as a electrolyte for solid-state battery applications. The thermal characteristics of the synthesized PCCSE were investigated using DSC (Karaman et al. 2019, Haridass et al. 2023). As shown in Fig. 3 , DSC thermograms were obtained for pure PEO, PVDF, their PEO/PVDF blend, and the composites PEO/PVDF-LiBO 3 and PEO/PVDF-LiBO 3 -LLZO. The analysis revealed distinct melting temperatures at 42.5°C (PEO), 48°C (PVDF), 45°C (PEO/PVDF blend), 94.5°C (PEO/PVDF-LiBO 3 ), and 100°C (PEO/PVDF-LiBO 3 -LLZO). The PEO/PVDF-LiBO 3 -LLZO composite exhibited a single, well-defined melting endotherm at 100°C, achieving the optimal balance of thermal stability and amorphous phase characteristics, which are essential for advanced solid-state electrolyte applications. FTIR spectroscopy is a powerful analytical technique used to investigate the functional groups, and ion-polymer interactions of PCCSE (Li et al. 2020). Fig. 4 shows the FTIR spectra of PEO, PVDF, PEO/PVDF, LiBO 3 , LLZO and (PEO/PVDF-LiBO 3 -LLZO). Upon the incorporation of the solid electrolyte LiBO 3 and the inorganic filler LLZO, the intensity the -OH bond (2880 cm -1 ), C – C bond (1068 cm -1 , 1111 cm -1 ) and the -CH 2 bond (1460 cm -1 ) decreased significantly, while adjacent peaks appeared at 830 cm -1 . These spectral modifications indicate that LiBO 3 and LLZO disrupt polymer crystallinity through weakened intermolecular interactions. The observed peak attenuation and shifts suggest the formation of amorphous domains that facilitate Li⁺ ion transport, a crucial characteristic for enhancing the performance of solid polymer electrolytes. The UV–Visible spectra in Fig. 5a illustrate the absorbance characteristics of PEO, PVDF, and LLZO, highlighting their maximum absorbance within the 200–1200 nm range (Sreekanth et al. 2019, Marceau et al. 2016). Fig. 5b presents the UV–Vis absorbance spectra of PEO/PVDF, PEO/PVDF-LiBO 3 , and PCCSE, revealing that the PEO/PVDF polymer blend matrix exhibits a strong absorption band at 215 nm, attributed to electronic transitions in the chromophore groups of PVDF and PEO. The PEO/PVDF-LiBO 3 composite shows a slightly shifted absorption band at 218 nm. In PCCSE, a strong and intense band appears at 225 nm, along with an additional peak at 283 nm, indicating interactions between the PBM, the solid electrolyte, and the LLZO filler. Moreover, PCCSE exhibits no absorption bands in the visible region, consistent with its transparent nature. The band gap values of PEO/PVDF, PEO/PVDF-LiBO 3 , and PEO/PVDF-LiBO 3 -LLZO are presented in Table 1, among the electrolytes, PCCSE possesses the lowest band gap, promoting better electron conduction. Table 1 The Band gaps values of PEO/PVDF, PEO/PVDF-LiBO 3 and PEO/PVDF-LiBO 3 -LLZO. Sample Band Gap (eV) PEO/PVDF 5.76 PEO/PVDF-LiBO 3 5.68 PEO/PVDF-LiBO 3 -LLZO 4.38 Chemical characteristic LSV was used to determine the electrochemical window, which is a critical factor in assessing the suitability of PCCSE for battery applications (Deng et al. 2015, Muzadi et al. 2023a). Fig. 6, presents the decomposition voltage of PEO/PVDF, PEO/PVDF-LiBO 3 , and PEO/PVDF-LiBO 3 -LLZO. The decomposition voltage of the polymer blend matrix (PBM) (PEO/PVDF) was 5.13 V . The introduction of the solid electrolyte LiBO 3 increased the decomposition voltage to 5.25 V , while further doping with the inorganic ceramic filler LLZO resulted in an even higher value of 5.33 V . [34] The Electrochemical Stability Window (ESW) and Electrochemical Window (EW) of PEO/PVDF, PEO/PVDF-LiBO 3 , and PEO/PVDF-LiBO 3 -LLZO PCCSE are summarized in Table 2 . Table 2 The Electrochemical Stability Window (ESW) and Electrochemical Window (EW) of the electrolytes. Sample Electrochemical Stability Window (ESW) Electrochemical Window (EW) (Reduction Potential – Oxidation Potential) PEO/PVDF 5.13 V 3.13 V PEO/PVDF-LiBO 3 5.25 V 3.25 V PEO/PVDF-LiBO 3 -LLZO 5.33 V 3.33 V The electrical behaviour of the system was evaluated using EIS (Suo et al. 2015, Koduru et al. 2016). Fig. 7, displays the Nyquist plots for the PEO/PVDF blend, PEO/PVDF-LiBO 3 and the composite (PEO/PVDF-LiBO 3 -LLZO). The impedance value (Z′) for the PEO/PVDF blend (PBM) is approximately 200 Ω, while for PEO/PVDF-LiBO 3 it it 180 Ω. In Contrast, the composite PCCSE (PEO/PVDF-LiBO 3 -LLZO) shows a significantly reduced Z′ value of 150 Ω. This reduction in impedance reflects a reduction in the total resistance of the system, which arises from the incorporation of LiBO 3 electrolyte and the inorganic ceramic filler LLZO. Owning to this, the ionic conductivity of the PCCSE, calculated from the resistance values obtained from the Nyquist plot, is determined to be 4.25 × 10⁻⁵ S/cm. The electrochemical performance of the prepared PCCSE was explored through charge-discharge tests using LiCoO₂ as the cathode and Li metal as the anode (Nguyen et al. 2025, Liang et al. 2018). PEO/PVDF-LiBO 3 -LLZO demonstrated distinct discharge and charge voltage platforms across current densities observed from 0.1 C to 2 C at 30 o C fig. 8(a). At 0.1 C, the discharge stable voltage curve is observed at 3.45 V, while the charge voltage curve shows a plateau around 3.48 V. An increase in current density leads to more significant potential variations over the entire electrochemical cycle. The discharge capacity of the cell is 148.5 mAh g⁻¹, 143.8 mAh g⁻¹, 135.6 mAh g⁻¹, 118.4 mAh g⁻¹, 75.5 mAh g⁻¹ at the rate of 0.1 C, 0.2 C, 0.5 C, 1C and 2C respectively. Fig. 8(b) illustrates the charging and discharging plateaus for the 1 st , 10 th , 50 th , 100 th and 200 th cycle. There is no significant difference in the specific capacity as the number of cycles increases. Fig. 8(c) exhibits the durability of the battery through cycling tests with electrolyte PEO/PVDF and PEO/PVDF-LiBO 3 -LLZO at 30°C and 0.1C rate. The maximum discharge capacity of the PCCSE is 147.3 mAh g⁻¹ in the initial cycle and decreases slightly to 145.2 mAh g⁻¹ after hundred cycles, demonstrating a stability of 95% of the initial capacity. The power capability performance of the battery with PCCSE, depicted in Fig. 8(d), illustrates the relationship between the specific discharge capacity and cycle number over a range of 0.1C to 2C. As the number of cycles increased, the specific capacity clearly decreases, which can be attributed to the limitations in Li⁺ diffusion within the electrode material. The cell cycle shows a stable discharge capacity above 140 mAh g⁻¹ at 0.1 C, 0.2 C and 0.5 C. The Charge and discharge capacity of the Li ǁ PEO/PVDF-LiBO 3 -LLZO ǁ LiCoO 2 at various C – rate at 30 o C is shown in the table 3. Table 3 The energy cycling capacity of the Li ǁ PEO/PVDF-LiBO 3 -LLZO ǁ LiCoO 2 at various C – rate at 30 o C C - rate 0.1 C 0.2 C 0.5 C 1 C 2 C Discharge Capacity (mAh g -1 ) 148.5 143.8 135.6 118.4 75.5 Charge Capacity (mAh g -1 ) 149.4 145.7 137.8 119.8 77.8 The electrochemical durability and long-term behavior of PCCSE with the Li anode were evaluated using Li || PCCSE || LiCoO 2 cells in a galvanostatic cycling test (Xue et al. 2020, Kannadasan et al. 2024). The potential variation profiles of the electrolytes, Li || PBM || LiCoO 2 (Fig. 9a) and Li || PCCSE || LiCoO 2 (Fig. 9b), were monitored throughout the duration in symmetrical Li cells. The cell system was maintained at a stable temperature of 30°C and subjected to a uniform current of 0.2 mA cm -2 . The symmetrical Li cell with Li || PBM || LiCoO 2 functioned for 300 hours, but a short-circuit phenomenon occurred after 180 hours due to uneven lithium electrodeposition, which typically leads reduced stability. In contrast, the symmetrical Li cell with Li || PCCSE || LiCoO 2 operated for 300 hours without encountering short circuits. The incorporation of the LiBO 3 electrolyte and LLZO ceramic filler contributed to the extended cycle life of the Li || PCCSE || LiCoO 2 cells by effectively reducing the growth of Li dendrite. The outcomes of the galvanostatic cycling experiments indicate that the PEO/PVDF-LiBO 3 -LLZO electrolyte promotes stable lithium deposition and inhibits dendrite lithium growth. Conclusion This study successfully developed and characterized a novel polymer composite ceramflux solid electrolyte (PCCSE), composed of PEO/PVDF, LiBO 3 , and LLZO, demonstrating strong potential for application in lithium-metal solid-state batteries (LSSBs). The incorporation of LLZO and LiBO 3 significantly reduced the crystallinity of the PBM, thereby enhancing the ion transport properties, mechanical strength, and electrochemical stability. Structural modifications were confirmed through XRD and DSC analyses, while FTIR and UV-Visible spectroscopy provided valuable insights into molecular interactions. Electrochemical evaluations, including impedance spectroscopy and linear sweep voltammetry, revealed an extended electrochemical stability window and reduced resistance. Full-cell testing using a LiCoO 2 cathode and a Li metal anode showed a substantial discharge capacity of 148.5 mAh g⁻¹ at 0.1C and 30 °C, with excellent cycling durability, retaining 95% of its capacity after hundred cycles. Moreover, the electrolyte efficiently suppressed lithium dendrite formation, contributing to enhanced safety and prolonged cycle life. These findings highlight the promise of PCCSE as a potential solid electrolyte for next-generation lithium-metal batteries, offering a balanced combination of high energy output, safety, and long-term stability. 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Energy Technol 8:2000444 Cite Share Download PDF Status: Published Journal Publication published 10 Jan, 2026 Read the published version in Chemical Papers → Version 1 posted Editorial decision: Minor revisions 12 Nov, 2025 Reviewers agreed at journal 22 Sep, 2025 Reviewers invited by journal 17 Sep, 2025 Editor assigned by journal 16 Sep, 2025 First submitted to journal 13 Sep, 2025 You are reading this latest preprint version Research Square lets you share your work early, gain feedback from the community, and start making changes to your manuscript prior to peer review in a journal. As a division of Research Square Company, we’re committed to making research communication faster, fairer, and more useful. We do this by developing innovative software and high quality services for the global research community. Our growing team is made up of researchers and industry professionals working together to solve the most critical problems facing scientific publishing. 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09:44:36","extension":"jpeg","order_by":2,"title":"Figure 2","display":"","copyAsset":false,"role":"figure","size":55911,"visible":true,"origin":"","legend":"\u003cp\u003e\u003cstrong\u003eXRD patterns of PEO, PVDF, PEO/PVDF (PBM), LiBO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e3\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e, LLZO, and PEO/PVDF-LiBO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e3\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e-LLZO (PCCSE).\u003c/strong\u003e\u003c/p\u003e","description":"","filename":"floatimage2.jpeg","url":"https://assets-eu.researchsquare.com/files/rs-7606253/v1/986e3d35b359d55dc8115386.jpeg"},{"id":92160708,"identity":"c4501a7f-ca0e-4f8b-b20d-f7e930ddca0e","added_by":"auto","created_at":"2025-09-25 10:00:36","extension":"png","order_by":3,"title":"Figure 3","display":"","copyAsset":false,"role":"figure","size":248339,"visible":true,"origin":"","legend":"\u003cp\u003e\u003cstrong\u003eDSC of a) PEO b) PVDF c) PEO/PVDF (PBM) d) PEO/PVDF-LiBO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e3\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e\u0026nbsp;d) PEO/PVDF-LiBO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e3\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e-LLZO (PCCSE).\u003c/strong\u003e\u003c/p\u003e","description":"","filename":"floatimage3.png","url":"https://assets-eu.researchsquare.com/files/rs-7606253/v1/197e4cb4a98bb2f8b91fa75c.png"},{"id":92159229,"identity":"532b17aa-923c-4aeb-8a29-ee5e0856829c","added_by":"auto","created_at":"2025-09-25 09:44:36","extension":"jpeg","order_by":4,"title":"Figure 4","display":"","copyAsset":false,"role":"figure","size":92473,"visible":true,"origin":"","legend":"\u003cp\u003e\u003cstrong\u003eFTIR spectra of PEO, PVDF, PEO/PVDF (PBM), LiBO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e3\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e, LLZO, and\u0026nbsp; PEO/PVDF-LiBO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e3\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e-LLZO (PCCSE).\u003c/strong\u003e\u003c/p\u003e","description":"","filename":"floatimage4.jpeg","url":"https://assets-eu.researchsquare.com/files/rs-7606253/v1/c358fef7d546044886d69b05.jpeg"},{"id":92160709,"identity":"d821bae5-8a8b-4e5b-acf4-42826a7af5f9","added_by":"auto","created_at":"2025-09-25 10:00:36","extension":"jpeg","order_by":5,"title":"Figure 5","display":"","copyAsset":false,"role":"figure","size":313119,"visible":true,"origin":"","legend":"\u003cp\u003e\u003cstrong\u003eUV-Visible Spectra of (a) PEO, PVDF, LLZO (b) PEO/PVDF (PBM), PEO/PVDF-LiBO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e3 \u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003eand PEO/PVDF-LiBO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e3\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e-LLZO (PCCSE)\u003c/strong\u003e\u003c/p\u003e","description":"","filename":"floatimage5.jpeg","url":"https://assets-eu.researchsquare.com/files/rs-7606253/v1/89a20d5ebd0ccf967b3ae17c.jpeg"},{"id":92159758,"identity":"f8a54b24-d21e-4d54-a046-441ea00e06fd","added_by":"auto","created_at":"2025-09-25 09:52:36","extension":"png","order_by":6,"title":"Figure 6","display":"","copyAsset":false,"role":"figure","size":51760,"visible":true,"origin":"","legend":"\u003cp\u003e\u003cstrong\u003eLinear Sweep Voltammetry of PEO/PVDF (PBM), PEO/PVDF-LiBO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e3\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e, and\u0026nbsp;PEO/PVDF-LiBO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e3\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e-LLZO (PCCSE).\u003c/strong\u003e\u003c/p\u003e","description":"","filename":"floatimage6.png","url":"https://assets-eu.researchsquare.com/files/rs-7606253/v1/9144dfeb34fa4e967eaf5bf8.png"},{"id":92159238,"identity":"c916902d-0b61-4570-a3bf-0551fdabca56","added_by":"auto","created_at":"2025-09-25 09:44:36","extension":"png","order_by":7,"title":"Figure 7","display":"","copyAsset":false,"role":"figure","size":54654,"visible":true,"origin":"","legend":"\u003cp\u003e\u003cstrong\u003eImpedance plots of PEO/PVDF (PBM), PEO/PVDF-LiBO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e3\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e and PEO/PVDF-LiBO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e3\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e-LLZO (PCCSE).\u003c/strong\u003e\u003c/p\u003e","description":"","filename":"floatimage7.png","url":"https://assets-eu.researchsquare.com/files/rs-7606253/v1/3a5c612420674c794df8b84a.png"},{"id":92159255,"identity":"19b06e1e-c73c-4fae-8157-1b1d2a7b554c","added_by":"auto","created_at":"2025-09-25 09:44:37","extension":"jpeg","order_by":8,"title":"Figure 8","display":"","copyAsset":false,"role":"figure","size":512919,"visible":true,"origin":"","legend":"\u003cp\u003e\u003cstrong\u003e(a) Specific capacity voltage curves of Li ǁ PEO/PVDF-LiBO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e3\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e-LLZO ǁ LiCoO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e2\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e with different C - rate, (b) Specific capacity voltage curves of Li ǁ PEO/PVDF-LiBO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e3\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e-LLZO ǁ LiCoO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e2\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e at the C-rate of 0.1 C, (c) cycling performance of PEO/PVDF (PBM), and PEO/PVDF-LiBO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e3\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e-LLZO (PCCSE) at 0.1C, (d) Discharge capacity with various cycle number.\u003c/strong\u003e\u003c/p\u003e","description":"","filename":"floatimage8.jpeg","url":"https://assets-eu.researchsquare.com/files/rs-7606253/v1/aaee3aac0f1b493ff4a744f3.jpeg"},{"id":92159766,"identity":"345d9a8d-5131-4ccf-ae9d-06c865ee793d","added_by":"auto","created_at":"2025-09-25 09:52:37","extension":"jpeg","order_by":9,"title":"Figure 9","display":"","copyAsset":false,"role":"figure","size":749682,"visible":true,"origin":"","legend":"\u003cp\u003e\u003cstrong\u003eGalvanostatic cycling test of (a) Li || PEO/PVDF (PBM) || LiCoO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e2\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e cell\u0026nbsp; (b) Li || PEO/PVDF-LiBO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e3\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e-LLZO (PCCSE) || LiCoO\u003c/strong\u003e\u003csub\u003e\u003cstrong\u003e2\u003c/strong\u003e\u003c/sub\u003e\u003cstrong\u003e cell.\u003c/strong\u003e\u003c/p\u003e","description":"","filename":"floatimage9.jpeg","url":"https://assets-eu.researchsquare.com/files/rs-7606253/v1/7f67ee1ec9ba160802440a66.jpeg"},{"id":100069447,"identity":"b848cad6-9e52-48a4-9e6c-8aed50d775fc","added_by":"auto","created_at":"2026-01-12 16:14:13","extension":"pdf","order_by":0,"title":"","display":"","copyAsset":false,"role":"manuscript-pdf","size":3349900,"visible":true,"origin":"","legend":"","description":"","filename":"manuscript.pdf","url":"https://assets-eu.researchsquare.com/files/rs-7606253/v1/bc1856c0-5348-4583-a302-1fbe8a169979.pdf"}],"financialInterests":"","formattedTitle":"Polymer–Ceramic Framework Stabilized Solid Electrolyte for Advanced Lithium-Ion Energy Storage","fulltext":[{"header":"Introduction","content":"\u003cp\u003eLithium-metal batteries (LMBs) are pivotal to modern energy storage, powering portable electronics with their high energy density, specific capacity, and extended cycle life. However, the surging demand for ultra-high-energy-density batteries, driven by the proliferation of smart devices and large-scale applications such as electric vehicles and grid storage, has intensified safety concerns (Ding et al. \u003cspan citationid=\"CR4\" class=\"CitationRef\"\u003e2019\u003c/span\u003e). These stem primarily from the volatility of organic liquid electrolytes, which pose risks of leakage and flammability, and the challenges associated with transitioning from graphite to lithium-metal anodes, notably lithium dendrite growth, which compromises battery safety and performance (Liu et al. \u003cspan citationid=\"CR22\" class=\"CitationRef\"\u003e2011\u003c/span\u003e). To address these issues, lithium-metal solid-state batteries (LSSBs) have emerged as a transformative solution, replacing liquid electrolytes with solid-state alternatives (Han et al. \u003cspan citationid=\"CR5\" class=\"CitationRef\"\u003e2020\u003c/span\u003e). LSSBs offer compelling advantages, including enhanced safety, wider electrochemical stability windows, broader operating temperature ranges, and the potential for compact, direct-stacking architectures, positioning them as a cornerstone for next-generation energy storage (Lee et al. \u003cspan citationid=\"CR14\" class=\"CitationRef\"\u003e2022\u003c/span\u003e, Li et al. \u003cspan citationid=\"CR15\" class=\"CitationRef\"\u003e2021\u003c/span\u003e).\u003c/p\u003e\u003cp\u003eAmong solid electrolyte materials, polyethylene oxide (PEO)-based polymers have garnered significant interest due to their ability to form stable Li-salt complexes that facilitate ion transport (D\u0026rsquo;Epifanio et al. \u003cspan citationid=\"CR1\" class=\"CitationRef\"\u003e2004\u003c/span\u003e). However, their semi-crystalline nature at room temperature limits ionic conductivity by restricting segmental chain mobility, while their modest mechanical strength fails to suppress lithium dendrite growth during cycling (Kannadasan et al. \u003cspan citationid=\"CR11\" class=\"CitationRef\"\u003e2024\u003c/span\u003e, Wang et al. \u003cspan citationid=\"CR37\" class=\"CitationRef\"\u003e2005\u003c/span\u003e). To overcome these limitations, blending PEO with polyvinylidene fluoride (PVDF) to form a polymer blend matrix (PBM) has proven effective (Nasir et al. \u003cspan citationid=\"CR27\" class=\"CitationRef\"\u003e2007\u003c/span\u003e, Xi et al. \u003cspan citationid=\"CR39\" class=\"CitationRef\"\u003e2006\u003c/span\u003e). PVDF contributes high mechanical strength, electrochemical stability, and favorable interactions with lithium salts, enhancing the thermal stability and amorphous content of the PEO-PVDF blend (Li et al. \u003cspan citationid=\"CR19\" class=\"CitationRef\"\u003e2025\u003c/span\u003e, Wu et al. \u003cspan citationid=\"CR38\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). This synergy improves ionic conductivity and electrode-electrolyte interfacial compatibility, yet achieving optimal ionic conductivity and dendrite suppression at ambient conditions remains a critical challenge.\u003c/p\u003e\u003cp\u003eTo further enhance performance, lithium perborate (LiBO\u003csub\u003e3\u003c/sub\u003e), a dimeric salt with water of hydration (Li\u003csub\u003e2\u003c/sub\u003e[B\u003csub\u003e2\u003c/sub\u003e(O\u003csub\u003e2\u003c/sub\u003e)\u003csub\u003e2\u003c/sub\u003e(OH)\u003csub\u003e4\u003c/sub\u003e]\u0026middot;4H\u003csub\u003e2\u003c/sub\u003eO), has been incorporated as a cost-effective, environmentally benign, non-toxic lithium salt and its gives hydrogen peroxide on hydration (Pandurangan et al. \u003cspan citationid=\"CR29\" class=\"CitationRef\"\u003e2024\u003c/span\u003e, Li et al. \u003cspan citationid=\"CR20\" class=\"CitationRef\"\u003e2024\u003c/span\u003e). LiBO\u003csub\u003e3\u003c/sub\u003eincreases the concentration of mobile lithium ions, disrupts ion pairing within the PBM, and reduces PEO crystallinity, thereby boosting ionic conductivity and electrochemical stability (Sampathkumar et al. \u003cspan citationid=\"CR33\" class=\"CitationRef\"\u003e2019\u003c/span\u003e). Its compatibility with PEO-PVDF blends further enhances miscibility and widens the operating voltage window, offering a sustainable alternative to conventional salts like LiClO\u003csub\u003e4\u003c/sub\u003e, LiTFSI, and LiBF\u003csub\u003e4\u003c/sub\u003e.\u003c/p\u003e\u003cp\u003eTo address mechanical and ionic conductivity limitations, lithium lanthanum zirconium oxide (LLZO), a garnet-structured ceramic, is integrated as a filler (Hegazy et al. \u003cspan citationid=\"CR7\" class=\"CitationRef\"\u003e2022\u003c/span\u003e, Hu et al. \u003cspan citationid=\"CR8\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). LLZO\u0026rsquo;s high ionic conductivity, exceptional mechanical strength, and stability against lithium metal provide additional ion conduction pathways, reduce polymer crystallinity, and effectively suppress dendrite growth. The synergistic combination of PEO, PVDF, LiBO\u003csub\u003e3\u003c/sub\u003e, and LLZO yields a polymer composite ceramflux solid electrolyte (PCCSE), which combines the flexibility and interfacial compatibility of the PBM, the enhanced conductivity and stability of LiBO\u003csub\u003e3\u003c/sub\u003e, and the mechanical and ionic transport benefits of LLZO.\u003c/p\u003e\u003cp\u003eThis study presents the synthesis and characterization of a novel PCCSE comprising PEO/PVDF, LiBO\u003csub\u003e3\u003c/sub\u003e, and LLZO, tailored for LSSBs with a lithium-metal anode and a lithium cobalt oxide (LiCoO\u003csub\u003e2\u003c/sub\u003e) cathode (Li et al. \u003cspan citationid=\"CR15\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). Emphasis is placed on elucidating the interfacial interactions among the PBM, LiBO\u003csub\u003e3\u003c/sub\u003e, and LLZO, which critically govern ion transport, mechanical properties, and electrochemical performance. By addressing the longstanding challenges of ionic conductivity, mechanical stability, and dendrite suppression, this PCCSE represents a significant advancement in LSSB technology, with far-reaching implications for electric vehicles, grid-scale energy storage, and the future of sustainable energy systems.\u003c/p\u003e"},{"header":"Experimental Section","content":"\u003cdiv id=\"Sec3\" class=\"Section2\"\u003e\u003ch2\u003eMaterials\u003c/h2\u003e\u003cp\u003eA combination of different chemicals was used to prepare the PCCSE material, such as Lithium carbonate (Li\u003csub\u003e2\u003c/sub\u003eCO\u003csub\u003e3\u003c/sub\u003e, from Sigma-Aldrich), Lanthanum oxide (La\u003csub\u003e2\u003c/sub\u003eO\u003csub\u003e3\u003c/sub\u003e, from Alfa Aesar), Ethylene glycol (C\u003csub\u003e2\u003c/sub\u003eH\u003csub\u003e6\u003c/sub\u003eO\u003csub\u003e2\u003c/sub\u003e, from Merck), Zirconium ethoxide (Zr(OC\u003csub\u003e2\u003c/sub\u003eH\u003csub\u003e5\u003c/sub\u003e)\u003csub\u003e4\u003c/sub\u003e, from Alfa Aesar), Dilute Nitric acid (HNO\u003csub\u003e3\u003c/sub\u003e, from Sigma-Aldrich), Citric acid (C\u003csub\u003e6\u003c/sub\u003eH\u003csub\u003e8\u003c/sub\u003eO\u003csub\u003e7\u003c/sub\u003e, from Sigma-Aldrich), Ethanol (C\u003csub\u003e2\u003c/sub\u003eH\u003csub\u003e5\u003c/sub\u003eOH, from Merck), Polyethylene oxide (PEO) from Merck, Polyvinylidene fluoride (PVDF, from Merck),), Dimethylformamide (DMF, from Merck), Lithium perborate tetrahydrate (LiBO\u003csub\u003e3\u003c/sub\u003e.4H\u003csub\u003e2\u003c/sub\u003eO, from Alfa Aesar). Only analytically pure, high-quality compounds were employed in this study (Patla et al. \u003cspan citationid=\"CR30\" class=\"CitationRef\"\u003e2018\u003c/span\u003e).\u003c/p\u003e\u003c/div\u003e\n\u003ch3\u003ePreparation of LiLaZrO (LLZO) powder\u003c/h3\u003e\n\u003cp\u003eA mixture of Li\u003csub\u003e2\u003c/sub\u003eCO\u003csub\u003e3\u003c/sub\u003e, La\u003csub\u003e2\u003c/sub\u003eO\u003csub\u003e3\u003c/sub\u003e, Zr(OC\u003csub\u003e2\u003c/sub\u003eH\u003csub\u003e5\u003c/sub\u003e)\u003csub\u003e4\u003c/sub\u003e, C\u003csub\u003e6\u003c/sub\u003eH\u003csub\u003e8\u003c/sub\u003eO\u003csub\u003e7\u003c/sub\u003e (as an organic complexing agent), and C\u003csub\u003e2\u003c/sub\u003eH\u003csub\u003e6\u003c/sub\u003eO\u003csub\u003e2\u003c/sub\u003e (as an organic medium) was prepared at a molar proportion of 7:3:4:28:14 as the reactant material. La\u003csub\u003e2\u003c/sub\u003eO\u003csub\u003e3\u003c/sub\u003e and Li\u003csub\u003e2\u003c/sub\u003eCO\u003csub\u003e3\u003c/sub\u003e were solubilised in HNO\u003csub\u003e3\u003c/sub\u003e, whereas Zr(OC\u003csub\u003e2\u003c/sub\u003eH\u003csub\u003e5\u003c/sub\u003e)\u003csub\u003e4\u003c/sub\u003e was dissolved in pure C\u003csub\u003e2\u003c/sub\u003eH\u003csub\u003e5\u003c/sub\u003eOH. The two liquid phases were then combined, and C\u003csub\u003e6\u003c/sub\u003eH\u003csub\u003e8\u003c/sub\u003eO\u003csub\u003e7\u003c/sub\u003e and C\u003csub\u003e2\u003c/sub\u003eH\u003csub\u003e6\u003c/sub\u003eO\u003csub\u003e2\u003c/sub\u003e subsequently incorporated into the formulation. The resulting mixture solution was vigorously stirred and heated at 70\u0026deg;C to evaporate the solvent. The synthesized sol was subsequently left to dry at 110\u0026deg;C for 12 hours. Upon drying, the gel obtained was subjected to heat at 600\u0026deg;C over 120 minutes periods, later on sintering at 800\u0026deg; C for 600 minutes to yield Li\u003csub\u003e7\u003c/sub\u003eLa\u003csub\u003e3\u003c/sub\u003eZr\u003csub\u003e2\u003c/sub\u003eO\u003csub\u003e12\u003c/sub\u003e powder (Sakamoto et al. \u003cspan citationid=\"CR32\" class=\"CitationRef\"\u003e2013\u003c/span\u003e).\u003c/p\u003e\n\u003ch3\u003ePreparation of PEO/PVDF-LiBO-LLZO\u003c/h3\u003e\n\u003cp\u003eA Stokes' solution-casting method was adopted to prepare PCCSE. Solutions of the PEO/PVDF PBM with a compositional mass ratio of 80/20 wt% were prepared by dissolving PEO (800 mg) and PVDF (200 mg) in conical glass flasks with stopper, followed by dissolving them in 15 ml of DMF at 80\u0026deg;C with constant stirring using magnetic stirrer. Thereafter, 30 wt% of LiBO\u003csub\u003e3\u003c/sub\u003e (0.30 g) in relation to the polymer blend, it was incorporated, followed by magnetic stirring to completely solvate the salt, resulting in polymeric blend matrix electrolyte ((80PEO/20PVDF)/30 wt% LiBO\u003csub\u003e3\u003c/sub\u003e). The required amount of LLZO (0.05 g), corresponding to 5 wt% with respect to the polymeric blend matrix electrolyte (1 g), was mixed in DMF and then combined with the polymeric blend matrix electrolyte solutions. The mixture was then cast onto Teflon-coated plates and placed on a heating plate at 75\u0026deg;C, allowing the solvent to evaporate completely. The films were then cooled to room temperature, then subjected to vacuum drying at 40\u0026deg;C for a day to remove any residual solvent, and stored in desiccators (Dhatarwal and Sengwa \u003cspan citationid=\"CR3\" class=\"CitationRef\"\u003e2019\u003c/span\u003e).\u003c/p\u003e\n\u003ch3\u003eCharacterization\u003c/h3\u003e\n\u003cdiv id=\"Sec7\" class=\"Section2\"\u003e\u003ch2\u003ePhysical characteristics\u003c/h2\u003e\u003cp\u003eThe crystal structures of the PEO, PVDF, PEO/PVDF, LiBO\u003csub\u003e3\u003c/sub\u003e, LLZO and PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO electrolytes were investigated using XRD analysis with a Rigaku RU-200B diffractometer and Cu Kα radiation (λ\u0026thinsp;=\u0026thinsp;1.5406 \u0026Aring;). XRD measurements, taken at 5\u0026deg;C/min scanning speed and 40 an operating voltage, covering a 2θ range of 10\u0026ndash;90\u0026deg;, revealing the crystalline phases. Differential scanning calorimetry (DSC) using a DSC 7 Perkin Elmer instrument elucidated the thermal behaviour and LiBO\u003csub\u003e3\u003c/sub\u003e solid electrolyte, and LLZO filler. (Tama\u0026ntilde;o-Machiavello et al. \u003cspan citationid=\"CR36\" class=\"CitationRef\"\u003e2015\u003c/span\u003e) DSC analysis provided insights into the phase transitions, melting points, and crystallization behaviour, highlighting influence the LLZO filler on the properties. FTIR by employing a Thermo Nicolet 380 spectrometer was used to analyze the molecular structure by measuring the infrared radiation absorption. A Cary 60 UV\u0026ndash;Vis spectrophotometer (Agilent, USA) was used for absorption analysis over the wavelength range of 200 \u0026minus;\u0026thinsp;1000 nm. The band gap of the electrolytes are calculated using\u003cdiv id=\"Equa\" class=\"Equation\"\u003e\u003cdiv format=\"TEX\" class=\"mathdisplay\" id=\"FileID_Equa\" name=\"EquationSource\"\u003e\n$$\\:E=\\:\\frac{1240}{\\lambda\\:}$$\u003c/div\u003e\u003c/div\u003e\u003c/p\u003e\u003cp\u003eWhere,\u003c/p\u003e\u003cp\u003eE\u0026thinsp;=\u0026thinsp;Band gap in eV\u003c/p\u003e\u003cp\u003e\u0026#120524; = wavelength in nm\u003c/p\u003e\u003cp\u003e1240 is the wavelength incident on 1eV (L\u0026oacute;pez and G\u0026oacute;mez \u003cspan citationid=\"CR23\" class=\"CitationRef\"\u003e2011\u003c/span\u003e).\u003c/p\u003e\u003c/div\u003e\u003cdiv id=\"Sec8\" class=\"Section2\"\u003e\u003ch2\u003eChemical characteristic\u003c/h2\u003e\u003cp\u003eLSV was used to examine the electrochemical behaviour and redox reaction kinetics by sweeping the working electrode potential linearly with time using an electrochemical analyzer (CHI-6650; CH Instruments) at 60\u003csup\u003eo\u003c/sup\u003e C at a rate of 1.0mVs\u003csup\u003e\u0026minus;\u0026thinsp;1\u003c/sup\u003e between the range of 2 and 6 V. Electrochemical impedance spectroscopy (EIS) provides insights into electrode-electrolyte interfaces and charge transfer processes using a small amplitude AC potential (Rathika et al. \u003cspan citationid=\"CR31\" class=\"CitationRef\"\u003e2017\u003c/span\u003e). Charge-discharge test and galvanostatic cycling tests were used to evaluate the electrochemical performance and cycling stability through repeated charging and discharging at controlled current densities. LSSBs batteries are fabricated with a lithium metal anode, lithium cobalt oxide (LiCoO\u003csub\u003e2\u003c/sub\u003e) cathode and prepared PCCSE (Li et al. \u003cspan citationid=\"CR15\" class=\"CitationRef\"\u003e2021\u003c/span\u003e).\u003c/p\u003e\u003c/div\u003e\n\u003ch3\u003eSchematic illustration of a lithium-metal solid-state battery\u003c/h3\u003e\n\u003cp\u003eA schematic illustration of a lithium-metal solid-state battery is shown in Fig.\u0026nbsp;\u003cspan refid=\"Fig1\" class=\"InternalRef\"\u003e1\u003c/span\u003e. The battery features a Li metal anode and lithium cobalt oxide (LiCoO\u003csub\u003e2\u003c/sub\u003e) cathode, with a polymer composite ceramflux solid electrolyte (PCCSE) in between. The PCCSE consists of a polymer blend matrix composed of polyethylene oxide (PEO) and polyvinylidene fluoride (PVDF), providing a flexible and process able medium for lithium-ion transport. Embedded within this matrix are lithium perborate (LiBO\u003csub\u003e3\u003c/sub\u003e), an environmentally friendly, cost-effective, and non-toxic solid electrolyte known for its mild oxidizing properties and wide applicability, and lithium lanthanum zirconium oxide (LLZO), a ceramic filler that significantly enhances ionic transport and thermal resistance. This configuration leverages the processability and flexibility of the PBM in conjunction with the high ion conductivity and thermal stability of ceramic materials, resulting in improved overall performance, safety, and longevity of the battery.\u003c/p\u003e\u003cp\u003e\u003c/p\u003e"},{"header":"Result and discussion","content":"\u003ch1\u003ePhysical characteristics\u003c/h1\u003e\n\u003cp\u003e\u003cstrong\u003eFig. 2\u003c/strong\u003e shows the XRD patterns of PEO, PVDF, PEO/PVDF blend, LiBO\u003csub\u003e3\u003c/sub\u003e, LLZO, and the PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO (PCCSE) (Jacob 1997). PEO exhibits characteristic sharp peaks at 19.2\u0026deg; and 23.6\u0026deg; (2\u0026theta;), confirming its semicrystalline nature, while PVDF shows distinct crystalline reflections at 18.3\u0026deg;, 20.5\u0026deg;, and 26\u0026deg; (2\u0026theta;). The PEO/PVDF blend demonstrates reduced peak intensities compared to the individual polymers, indicating a suppression of PEO crystallinity due to intermolecular interactions between the two polymers. Upon the incorporation of LiBO\u003csub\u003e3\u0026nbsp;\u003c/sub\u003eelectrolyte and LLZO fillers into the PEO-PVDF matrix, the PCCSE shows further reduction in crystallinity, along with new diffraction peaks corresponding to the ceramic phases. These results confirm that the PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO composite effectively suppresses crystallinity and promotes phase integration, suggesting strong polymer-ceramic interactions that enhance its performance as a electrolyte for solid-state battery applications.\u003c/p\u003e\n\u003cp\u003eThe thermal characteristics of the synthesized PCCSE were investigated using DSC (Karaman et al. 2019, Haridass et al. 2023). As shown in \u003cstrong\u003eFig. 3\u003c/strong\u003e, DSC thermograms were obtained for pure PEO, PVDF, their PEO/PVDF blend, and the composites PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e and PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO. The analysis revealed distinct melting temperatures at 42.5\u0026deg;C (PEO), 48\u0026deg;C (PVDF), 45\u0026deg;C (PEO/PVDF blend), 94.5\u0026deg;C (PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e), and 100\u0026deg;C (PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO). The PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO composite exhibited a single, well-defined melting endotherm at 100\u0026deg;C, achieving the optimal balance of thermal stability and amorphous phase characteristics, which are essential for advanced solid-state electrolyte applications.\u003c/p\u003e\n\u003cp\u003eFTIR spectroscopy is a powerful analytical technique used to investigate the functional groups, and ion-polymer interactions of PCCSE (Li et al. 2020). Fig. 4 shows the FTIR spectra of PEO, PVDF, PEO/PVDF, LiBO\u003csub\u003e3\u003c/sub\u003e, LLZO and (PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO). Upon the incorporation of the solid electrolyte LiBO\u003csub\u003e3\u003c/sub\u003e and the inorganic filler LLZO, the intensity the -OH bond (2880 cm\u003csup\u003e-1\u003c/sup\u003e), C \u0026ndash; C bond (1068 cm\u003csup\u003e-1\u003c/sup\u003e, 1111 cm\u003csup\u003e-1\u003c/sup\u003e) and the -CH\u003csub\u003e2\u003c/sub\u003e bond (1460 cm\u003csup\u003e-1\u003c/sup\u003e) decreased significantly, while adjacent peaks appeared at 830 cm\u003csup\u003e-1\u003c/sup\u003e. These spectral modifications indicate that LiBO\u003csub\u003e3\u003c/sub\u003e and LLZO disrupt polymer crystallinity through weakened intermolecular interactions. The observed peak attenuation and shifts suggest the formation of amorphous domains that facilitate Li⁺ ion transport, a crucial characteristic for enhancing the performance of solid polymer electrolytes.\u003c/p\u003e\n\u003cp\u003eThe UV\u0026ndash;Visible spectra in Fig. 5a illustrate the absorbance characteristics of PEO, PVDF, and LLZO, highlighting their maximum absorbance within the 200\u0026ndash;1200 nm range (Sreekanth et al. 2019,\u0026nbsp;Marceau et al. 2016). Fig. 5b presents the UV\u0026ndash;Vis absorbance spectra of PEO/PVDF, PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e, and PCCSE, revealing that the PEO/PVDF polymer blend matrix exhibits a strong absorption band at 215 nm, attributed to electronic transitions in the chromophore groups of PVDF and PEO. The PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e composite shows a slightly shifted absorption band at 218 nm. In PCCSE, a strong and intense band appears at 225 nm, along with an additional peak at 283 nm, indicating interactions between the PBM, the solid electrolyte, and the LLZO filler. Moreover, PCCSE exhibits no absorption bands in the visible region, consistent with its transparent nature. The band gap values of PEO/PVDF, PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e, and PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO are presented in Table 1, among the electrolytes, PCCSE possesses the lowest band gap, promoting better electron conduction.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eTable 1\u0026nbsp;\u003c/strong\u003e\u003cstrong\u003eThe Band gaps values of PEO/PVDF, PEO/PVDF-LiBO\u003csub\u003e3\u0026nbsp;\u003c/sub\u003eand PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO.\u0026nbsp;\u003c/strong\u003e\u003c/p\u003e\n\u003ctable border=\"1\" cellspacing=\"0\" cellpadding=\"0\"\u003e\n \u003ctbody\u003e\n \u003ctr\u003e\n \u003ctd style=\"width: 227px;\"\u003e\n \u003cp\u003e\u003cstrong\u003eSample\u003c/strong\u003e\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 186px;\"\u003e\n \u003cp\u003e\u003cstrong\u003eBand Gap (eV)\u003c/strong\u003e\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003ctr\u003e\n \u003ctd style=\"width: 227px;\"\u003e\n \u003cp\u003ePEO/PVDF\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 186px;\"\u003e\n \u003cp\u003e\u003cstrong\u003e5.76\u003c/strong\u003e\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003ctr\u003e\n \u003ctd style=\"width: 227px;\"\u003e\n \u003cp\u003ePEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 186px;\"\u003e\n \u003cp\u003e\u003cstrong\u003e5.68\u003c/strong\u003e\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003ctr\u003e\n \u003ctd style=\"width: 227px;\"\u003e\n \u003cp\u003ePEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 186px;\"\u003e\n \u003cp\u003e\u003cstrong\u003e4.38\u003c/strong\u003e\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003c/tbody\u003e\n\u003c/table\u003e\n\u003cp\u003e\u0026nbsp;\u003cstrong\u003eChemical characteristic\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eLSV was used to determine the electrochemical window, which is a critical factor in assessing the suitability of PCCSE for battery applications (Deng et al. 2015, Muzadi et al. 2023a). Fig. 6, presents the decomposition voltage of PEO/PVDF, PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e, and PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO. The decomposition voltage of the polymer blend matrix (PBM) \u003cstrong\u003e(PEO/PVDF)\u003c/strong\u003e was \u003cstrong\u003e5.13 V\u003c/strong\u003e. The introduction of the solid electrolyte \u003cstrong\u003eLiBO\u003c/strong\u003e\u003csub\u003e3\u003c/sub\u003e increased the decomposition voltage to \u003cstrong\u003e5.25 V\u003c/strong\u003e, while further doping with the inorganic ceramic filler \u003cstrong\u003eLLZO\u003c/strong\u003e resulted in an even higher value of \u003cstrong\u003e5.33 V\u003c/strong\u003e. [34] The \u003cstrong\u003eElectrochemical Stability Window (ESW)\u003c/strong\u003e and \u003cstrong\u003eElectrochemical Window (EW)\u003c/strong\u003e of PEO/PVDF, PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e, and PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO PCCSE are summarized in \u003cstrong\u003eTable 2\u003c/strong\u003e.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eTable 2 \u0026nbsp;\u003c/strong\u003e\u003cstrong\u003eThe Electrochemical Stability Window (ESW) and Electrochemical Window (EW) of the electrolytes.\u003c/strong\u003e\u003c/p\u003e\n\u003ctable border=\"1\" cellspacing=\"0\" cellpadding=\"0\" width=\"666\"\u003e\n \u003ctbody\u003e\n \u003ctr\u003e\n \u003ctd style=\"width: 209px;\"\u003e\n \u003cp\u003e\u003cstrong\u003eSample\u003c/strong\u003e\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 209px;\"\u003e\n \u003cp\u003e\u003cstrong\u003eElectrochemical Stability Window (ESW)\u003c/strong\u003e\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 247px;\"\u003e\n \u003cp\u003e\u003cstrong\u003eElectrochemical Window (EW)\u0026nbsp;\u003c/strong\u003e(Reduction Potential \u0026ndash; Oxidation Potential)\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003ctr\u003e\n \u003ctd style=\"width: 209px;\"\u003e\n \u003cp\u003ePEO/PVDF\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 209px;\"\u003e\n \u003cp\u003e5.13 V\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 247px;\"\u003e\n \u003cp\u003e3.13 V\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003ctr\u003e\n \u003ctd style=\"width: 209px;\"\u003e\n \u003cp\u003ePEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 209px;\"\u003e\n \u003cp\u003e5.25 V\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 247px;\"\u003e\n \u003cp\u003e3.25 V\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003ctr\u003e\n \u003ctd style=\"width: 209px;\"\u003e\n \u003cp\u003ePEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 209px;\"\u003e\n \u003cp\u003e5.33 V\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 247px;\"\u003e\n \u003cp\u003e3.33 V\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003c/tbody\u003e\n\u003c/table\u003e\n\u003cp\u003eThe electrical behaviour of the system was evaluated using EIS (Suo et al. 2015, Koduru et al. 2016). Fig. 7, displays the Nyquist plots for the PEO/PVDF blend, PEO/PVDF-LiBO\u003csub\u003e3\u0026nbsp;\u003c/sub\u003eand the composite (PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO). The impedance value (Z\u0026prime;) for the PEO/PVDF blend (PBM) is approximately 200 Ω, while for PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e it it 180 Ω. In Contrast, the composite PCCSE (PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO) shows a significantly reduced\u0026nbsp;Z\u0026prime;\u0026nbsp;value of 150 Ω. This reduction in impedance reflects a reduction in the total resistance of the system, which arises from the incorporation of LiBO\u003csub\u003e3\u003c/sub\u003e electrolyte and the inorganic ceramic filler LLZO. Owning to this, the ionic conductivity of the PCCSE, calculated from the resistance values obtained from the Nyquist plot, is determined to be 4.25 \u0026times; 10⁻⁵ S/cm.\u003c/p\u003e\n\u003cp\u003eThe electrochemical performance of the prepared PCCSE was explored through charge-discharge tests using LiCoO₂ as the cathode and Li metal as the anode (Nguyen et al. 2025, Liang et al. 2018). PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO demonstrated distinct discharge and charge voltage platforms across current densities observed from 0.1 C to 2 C at 30\u003csup\u003eo\u003c/sup\u003e C fig. 8(a). At 0.1 C, the discharge stable voltage curve is observed at 3.45 V, while the charge voltage curve shows a plateau around 3.48 V. An increase in current density leads to more significant potential variations over the entire electrochemical cycle. The discharge capacity of the cell is 148.5 mAh g⁻\u0026sup1;, 143.8 mAh g⁻\u0026sup1;, 135.6 mAh g⁻\u0026sup1;, 118.4 mAh g⁻\u0026sup1;, 75.5 mAh g⁻\u0026sup1; at the rate of 0.1 C, 0.2 C, 0.5 C, 1C and 2C respectively. Fig. 8(b) illustrates the charging and discharging plateaus for the 1\u003csup\u003est\u003c/sup\u003e, 10\u003csup\u003eth\u003c/sup\u003e, 50\u003csup\u003eth\u003c/sup\u003e, 100\u003csup\u003eth\u003c/sup\u003e and 200\u003csup\u003eth\u003c/sup\u003e cycle. There is no significant difference in the specific capacity as the number of cycles increases. Fig. 8(c) exhibits the durability of the battery through cycling tests with electrolyte PEO/PVDF and PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO at 30\u0026deg;C and 0.1C rate. The maximum discharge capacity of the PCCSE is 147.3 mAh g⁻\u0026sup1; in the initial cycle and decreases slightly to 145.2 mAh g⁻\u0026sup1; after hundred cycles, demonstrating a stability of 95% of the initial capacity. \u0026nbsp;The power capability performance of the battery with PCCSE, depicted in Fig. 8(d), illustrates the relationship between the specific discharge capacity and cycle number over a range of 0.1C to 2C. As the number of cycles increased, the specific capacity clearly decreases, which can be attributed to the limitations in Li⁺ diffusion within the electrode material. The cell cycle shows a stable discharge capacity above 140 mAh g⁻\u0026sup1; at 0.1 C, 0.2 C and 0.5 C. The Charge and discharge capacity of the Li ǁ PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO ǁ LiCoO\u003csub\u003e2\u003c/sub\u003e at various C \u0026ndash; rate at 30\u003csup\u003eo\u003c/sup\u003e C is shown in the table 3.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eTable 3\u0026nbsp;\u003c/strong\u003e\u003cstrong\u003eThe energy cycling capacity of the Li ǁ PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO ǁ LiCoO\u003csub\u003e2\u003c/sub\u003e at various C \u0026ndash; rate at 30\u003csup\u003eo\u003c/sup\u003e C\u003c/strong\u003e\u003c/p\u003e\n\u003ctable border=\"1\" cellspacing=\"0\" cellpadding=\"0\" width=\"624\"\u003e\n \u003ctbody\u003e\n \u003ctr\u003e\n \u003ctd style=\"width: 236px;\"\u003e\n \u003cp\u003e\u003cstrong\u003eC - rate\u003c/strong\u003e\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 66px;\"\u003e\n \u003cp\u003e\u003cstrong\u003e0.1 C\u003c/strong\u003e\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 85px;\"\u003e\n \u003cp\u003e\u003cstrong\u003e0.2 C\u003c/strong\u003e\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 85px;\"\u003e\n \u003cp\u003e\u003cstrong\u003e0.5 C\u003c/strong\u003e\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 76px;\"\u003e\n \u003cp\u003e\u003cstrong\u003e1 C\u003c/strong\u003e\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 76px;\"\u003e\n \u003cp\u003e\u003cstrong\u003e2 C\u003c/strong\u003e\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003ctr\u003e\n \u003ctd style=\"width: 236px;\"\u003e\n \u003cp\u003e\u003cstrong\u003eDischarge Capacity\u003c/strong\u003e (mAh g\u003csup\u003e-1\u003c/sup\u003e)\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 66px;\"\u003e\n \u003cp\u003e148.5\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 85px;\"\u003e\n \u003cp\u003e143.8\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 85px;\"\u003e\n \u003cp\u003e135.6\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 76px;\"\u003e\n \u003cp\u003e118.4\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 76px;\"\u003e\n \u003cp\u003e75.5\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003ctr\u003e\n \u003ctd style=\"width: 236px;\"\u003e\n \u003cp\u003e\u003cstrong\u003eCharge Capacity\u003c/strong\u003e\u0026nbsp; (mAh g\u003csup\u003e-1\u003c/sup\u003e)\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 66px;\"\u003e\n \u003cp\u003e149.4\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 85px;\"\u003e\n \u003cp\u003e145.7\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 85px;\"\u003e\n \u003cp\u003e137.8\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 76px;\"\u003e\n \u003cp\u003e119.8\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd style=\"width: 76px;\"\u003e\n \u003cp\u003e77.8\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003c/tbody\u003e\n\u003c/table\u003e\n\u003cp\u003eThe electrochemical durability and long-term behavior of PCCSE with the Li anode were evaluated using Li || PCCSE || LiCoO\u003csub\u003e2\u003c/sub\u003e cells in a galvanostatic cycling test (Xue et al. 2020, Kannadasan et al. 2024). The potential variation profiles of the electrolytes, Li || PBM || LiCoO\u003csub\u003e2\u003c/sub\u003e (Fig. 9a) and Li || PCCSE || LiCoO\u003csub\u003e2\u003c/sub\u003e (Fig. 9b), were monitored throughout the duration in symmetrical Li cells. The cell system was maintained at a stable temperature of 30\u0026deg;C and subjected to a uniform current of 0.2 mA cm\u003csup\u003e-2\u003c/sup\u003e. The symmetrical Li cell with Li || PBM || LiCoO\u003csub\u003e2\u003c/sub\u003e functioned for 300 hours, but a short-circuit phenomenon occurred after 180 hours due to uneven lithium electrodeposition, which typically leads reduced stability. In contrast, the symmetrical Li cell with Li || PCCSE || LiCoO\u003csub\u003e2\u003c/sub\u003e operated for 300 hours without encountering short circuits. The incorporation of the LiBO\u003csub\u003e3\u003c/sub\u003e electrolyte and LLZO ceramic filler contributed to the extended cycle life of the Li || PCCSE || LiCoO\u003csub\u003e2\u003c/sub\u003e cells by effectively reducing the growth of Li dendrite. The outcomes of the galvanostatic cycling experiments indicate that the PEO/PVDF-LiBO\u003csub\u003e3\u003c/sub\u003e-LLZO electrolyte promotes stable lithium deposition and inhibits dendrite lithium growth.\u003c/p\u003e"},{"header":"Conclusion","content":"\u003cp\u003eThis study successfully developed and characterized a novel polymer composite ceramflux solid electrolyte (PCCSE), composed of PEO/PVDF, LiBO\u003csub\u003e3\u003c/sub\u003e, and LLZO, demonstrating strong potential for application in lithium-metal solid-state batteries (LSSBs). The incorporation of LLZO and LiBO\u003csub\u003e3\u003c/sub\u003e significantly reduced the crystallinity of the PBM, thereby enhancing the ion transport properties, mechanical strength, and electrochemical stability. Structural modifications were confirmed through XRD and DSC analyses, while FTIR and UV-Visible spectroscopy provided valuable insights into molecular interactions. Electrochemical evaluations, including impedance spectroscopy and linear sweep voltammetry, revealed an extended electrochemical stability window and reduced resistance. Full-cell testing using a LiCoO\u003csub\u003e2\u003c/sub\u003e cathode and a Li metal anode showed a substantial discharge capacity of 148.5 mAh g⁻\u0026sup1; at 0.1C and 30 \u0026deg;C, with excellent cycling durability, retaining 95% of its capacity after hundred cycles. Moreover, the electrolyte efficiently suppressed lithium dendrite formation, contributing to enhanced safety and prolonged cycle life. These findings highlight the promise of PCCSE as a potential solid electrolyte for next-generation lithium-metal batteries, offering a balanced combination of high energy output, safety, and long-term stability. The development of such materials marks a significant step toward safer, high-performance energy storage solutions, with important implications for sustainable transportation and portable electronic technologies.\u003c/p\u003e"},{"header":"Declarations","content":"\u003cp\u003e\u003cstrong\u003eCRediT authorship contribution statement\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eIlakkiya Pandurangan: Manuscript preparation, validation of findings and conceptual planning. Muthukumaran Balakrishnan: Manuscript reviewing and editing, Supervision, Methodology, and investigative work.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eDeclaration of competing interest\u0026nbsp;\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eThe authors declare that they have no competing interests.\u003c/p\u003e"},{"header":"References","content":"\u003col\u003e\n\u003cli\u003eD\u0026rsquo;Epifanio A, Traversa E, Croce F, Serraino Fiory F, Scrosati B, Licoccia S (2004) Metallic-lithium, LiFePO4-based polymer battery using PEO\u0026ndash;ZrO2 nanocomposite polymer electrolyte. J Appl Electrochem 34:403\u0026ndash;408\u003c/li\u003e\n\u003cli\u003eDeng F, Wang X, He D, Hu J, Gong C, Ye YS, et al. (2015) Microporous polymer electrolyte based on PVDF/PEO star polymer blends for lithium-ion batteries. J Membr Sci 491:82\u0026ndash;89\u003c/li\u003e\n\u003cli\u003eDhatarwal P, Sengwa RJ (2019) Dielectric relaxation, Li-ion transport, electrochemical, and structural behaviour of PEO/PVDF/LiClO4/TiO2/PC-based plasticized nanocomposite solid polymer electrolyte films. Compos Commun 17:182\u0026ndash;191\u003c/li\u003e\n\u003cli\u003eDing Y, Yu A, Lu J, Chen Z, Cano ZP (2019) Automotive Li-ion batteries: Current status and future perspectives. Electrochem Energy Rev 2:1\u0026ndash;28\u003c/li\u003e\n\u003cli\u003eHan L, Zhu J, Lehmann ML, Saito T, Tang X, Liu T, et al. (2020) Recent developments and challenges in hybrid solid electrolytes for lithium-ion batteries. Front Energy Res 8:202\u003c/li\u003e\n\u003cli\u003eHaridass R, Augustin N, Brahmadesam Thoopul Srinivasa Raghava R, Annamalai PK, Sabu A (2023) Effect of polyvinylpyrrolidone on the structure development, electrical, thermal, and wetting properties of polyvinylidene fluoride\u0026ndash;expanded graphite nanocomposites. ACS Omega 9:178\u0026ndash;195\u003c/li\u003e\n\u003cli\u003eHegazy A, Higashiya S, Efstathiadis H, Mckinney J (2022) Evaluation of porous lithium lanthanum zirconium oxide (LLZO) anode host structures for Li-metal batteries. Electrochem Soc Meet Abstr MA2022-02:272\u003c/li\u003e\n\u003cli\u003eHu Y, Luo L, Feng T, Zhang L, Xu L (2022) Probing the phase transition during the formation of lithium lanthanum zirconium oxide solid electrolyte. ACS Appl Mater Interfaces 14:41978\u0026ndash;41987\u003c/li\u003e\n\u003cli\u003eJacob MME (1997) Effect of PEO addition on the electrolytic and thermal properties of PVDF\u0026ndash;LiClO4 polymer electrolytes. Solid State Ionics 104:267\u0026ndash;276\u003c/li\u003e\n\u003cli\u003eKannadasan M, Sathiasivan K, Pandurangan I, Balakrishnan M (2024) Synergistic nanocomposite polymer electrolytes for advanced all-solid-state sodium-ion batteries. Int J Hydrogen Energy 78:634\u0026ndash;641\u003c/li\u003e\n\u003cli\u003eKannadasan M, Varuvel EG, Sathiasivan K, Balakrishnan M, Subramanian B (2024) Crafting high-performance polymer-integrated solid electrolyte for solid-state sodium-ion batteries. Energy Storage 6:636\u003c/li\u003e\n\u003cli\u003eKaraman B, Bozkurt A, \u0026Ccedil;evik E (2019) Novel flexible Li-doped PEO/copolymer electrolytes for supercapacitor application. Ionics 25:1773\u0026ndash;1781\u003c/li\u003e\n\u003cli\u003eKoduru HK, Zhao X-Z, Scaramuzza N, Iliev MT, Karashanova D, Vlakhov T, et al. (2016) Investigations on poly(ethylene oxide) (PEO)-blend based solid polymer electrolytes for sodium-ion batteries. J Phys Conf Ser 764:012006\u003c/li\u003e\n\u003cli\u003eLee MJ, Lee YJ, Han J, Kim BJ, Lee SW, Lee K, et al. (2022) Elastomeric electrolytes for high-energy solid-state lithium batteries. Nature 601:217\u0026ndash;222\u003c/li\u003e\n\u003cli\u003eLi C, Zhang Z, Miao X, Wang C, Zhang S, Yin L, et al. (2021) Designing lithium argyrodite solid-state electrolytes for high-performance all-solid-state lithium batteries. Batteries Supercaps 5:1\u0026ndash;10\u003c/li\u003e\n\u003cli\u003eLi J, Qiu Y, Yang K, Chen P, Sun J, Hong Y, et al. (2021) Structural origin of the high-voltage instability of lithium cobalt oxide. Nat Nanotechnol 16:599\u0026ndash;605\u003c/li\u003e\n\u003cli\u003eLi J, Zhu K, Wang J, Yan K, Liu J, Yao Z, et al. (2020) Optimisation of conductivity of PEO/PVDF-based solid polymer electrolytes in all-solid-state Li-ion batteries. Mater Technol 37:240\u0026ndash;247\u003c/li\u003e\n\u003cli\u003eLi L, Deng Y, Duan H, Qian Y, Chen G (2021) LiF and LiNO3 as synergistic additives for PEO\u0026ndash;PVDF/LLZTO-based composite electrolyte towards high-voltage lithium batteries with dual-interfaces stability. J Energy Chem 65:319\u0026ndash;328\u003c/li\u003e\n\u003cli\u003eLi Y, Yuan W, Hu Z, Shen Y, Wu G, Cong F, et al. (2025) Constructing PVDF-based polymer electrolyte for lithium metal batteries by polymer-induced phase structure adjustment strategy. Adv Funct Mater 35:24763\u003c/li\u003e\n\u003cli\u003eLi Z, He X, Wang L, Huang X (2024) Lithium bis(trifluoromethanesulfonyl)imide (LiTFSI): A prominent lithium salt in lithium-ion battery electrolytes \u0026ndash; fundamentals, progress, and future perspectives. Adv Funct Mater 34:8319\u003c/li\u003e\n\u003cli\u003eLiang YF, Xia Y, Zhang SZ, Wang XL, Xia XH, Gu CD, et al. (2018) A preeminent gel blending polymer electrolyte of poly(vinylidene fluoride-hexafluoropropylene)\u0026ndash;poly(propylene carbonate) for solid-state lithium-ion batteries. Electrochim Acta 296:1064\u0026ndash;1069\u003c/li\u003e\n\u003cli\u003eLiu XH, Sullivan JP, Zhang LQ, Kushima A, Huang JY, Ye ZZ, et al. (2011) Lithium fiber growth on the anode in a nanowire lithium-ion battery during charging. Appl Phys Lett 98:183107\u003c/li\u003e\n\u003cli\u003eL\u0026oacute;pez R, G\u0026oacute;mez R (2011) Band-gap energy estimation from diffuse reflectance measurements on sol\u0026ndash;gel and commercial TiO2: A comparative study. J Sol-Gel Sci Technol 61:1\u0026ndash;7\u003c/li\u003e\n\u003cli\u003eMarceau H, Kim C-S, Paolella A, Ladouceur S, Lagac\u0026eacute; M, Chaker M, et al. (2016) In operando scanning electron microscopy and ultraviolet\u0026ndash;visible spectroscopy studies of lithium/sulfur cells using all solid-state polymer electrolyte. J Power Sources 319:247\u0026ndash;254\u003c/li\u003e\n\u003cli\u003eMuzadi H, Kamalia NZ, Lestariningsih T, Astuti Y (2023) Effect of LiTFSI electrolyte salt composition on characteristics of PVDF\u0026ndash;PEO\u0026ndash;LiTFSI-based solid polymer electrolyte (SPE) for lithium-ion battery. Molekul 18:98\u003c/li\u003e\n\u003cli\u003eMuzadi H, Kamalia NZ, Lestariningsih T, Astuti Y (2023) Effect of LiTFSI electrolyte salt composition on characteristics of PVDF\u0026ndash;PEO\u0026ndash;LiTFSI-based solid polymer electrolyte (SPE) for lithium-ion battery. Molekul 18:98\u003c/li\u003e\n\u003cli\u003eNasir M, Matsumoto H, Danno T, Minagawa M, Tanioka A, Horibe H (2007) Preparation of porous PVDF nanofiber from PVDF/PVP blend by electrospray deposition. Polym J 39:1060\u0026ndash;1064\u003c/li\u003e\n\u003cli\u003eNguyen HBT, Ding L, Pohle B, Schmeida T, Nguyen HBA, Mikhailova D (2025) Ternary PEO/PVDF-HFP-based polymer electrolytes for Li-ion batteries. Batteries 11:45\u003c/li\u003e\n\u003cli\u003ePandurangan I, Kannadasan M, Sathiasivan K, Aarimuthu G, Balakrishnan M (2024) Lithium perborate-based composite polymer electrolytes for all-solid-state lithium-ion batteries: Performance enhancement and stability. J Solid State Electrochem 28:1\u0026ndash;12\u003c/li\u003e\n\u003cli\u003ePatla SK, Asokan K, Karmakar S, Ray R (2018) Investigation of ionic conduction in PEO\u0026ndash;PVDF based blend polymer electrolytes. J Appl Phys 123:125102\u003c/li\u003e\n\u003cli\u003eRathika R, Padmaraj O, Suthanthiraraj SA (2017) Electrical conductivity and dielectric relaxation behaviour of PEO/PVdF-based solid polymer blend electrolytes for zinc battery applications. Ionics 24:243\u0026ndash;255\u003c/li\u003e\n\u003cli\u003eSakamoto J, Kim H, Wolfenstine J, Rangasamy E, Kim Y (2013) Synthesis of nano-scale fast ion conducting cubic Li7La3Zr2O12. Nanotechnology 24:424005\u003c/li\u003e\n\u003cli\u003eSampathkumar L, Selvasekarapandian S, Chitra R, Muthukrishnan M, Christopher Selvin P, Perumal P (2019) Synthesis and characterization of biopolymer electrolyte based on tamarind seed polysaccharide, lithium perchlorate and ethylene carbonate for electrochemical applications. Ionics 25:1067\u0026ndash;1082\u003c/li\u003e\n\u003cli\u003eSreekanth K, Madhava Kumar Y, Ramu C, Gopal NO, Siddaiah T (2019) Optical and electrical conductivity studies of VO2+ doped polyvinyl pyrrolidone (PVP) polymer electrolytes. J Sci Adv Mater Devices 4:230\u0026ndash;236\u003c/li\u003e\n\u003cli\u003eSuo L, Fan X, Xu K, Wang C, Olguin M, Gao T, et al. (2015) \u0026ldquo;Water-in-salt\u0026rdquo; electrolyte enables high-voltage aqueous lithium-ion chemistries. Science 350:938\u0026ndash;943\u003c/li\u003e\n\u003cli\u003eTama\u0026ntilde;o-Machiavello MN, Costa CM, Molina-Mateo J, Torregrosa-Cabanilles C, Meseguer-Due\u0026ntilde;as JM, Kalkura SN, et al. (2015) Phase morphology and crystallinity of poly(vinylidene fluoride)/poly(ethylene oxide) piezoelectric blend membranes. Mater Today Commun 4:214\u0026ndash;221\u003c/li\u003e\n\u003cli\u003eWang GX, Yang L, Liu HK, Dou SX, Wang JZ (2005) Enhancement of ionic conductivity of PEO based polymer electrolyte by the addition of nanosize ceramic powders. J Nanosci Nanotechnol 5:1135\u0026ndash;1140\u003c/li\u003e\n\u003cli\u003eWu Y, Li Y, Wang Y, Liu Q, Chen Q, Chen M (2021) Advances and prospects of PVDF based polymer electrolytes. J Energy Chem 64:62\u0026ndash;84\u003c/li\u003e\n\u003cli\u003eXi J, Qiu X, Chen L (2006) PVDF\u0026ndash;PEO/ZSM-5 based composite microporous polymer electrolyte with novel pore configuration and ionic conductivity. Solid State Ionics 177:709\u0026ndash;713\u003c/li\u003e\n\u003cli\u003eXue X, Chen Y, Zhang X, Chen S, Lin J, Zhang Y, et al. (2020) Boosting the performance of solid-state lithium battery based on hybridizing micron-sized LATP in a PEO/PVDF-HFP heterogeneous polymer matrix. Energy Technol 8:2000444\u003c/li\u003e\n\u003c/ol\u003e"}],"fulltextSource":"","fullText":"","funders":[],"hasAdminPriorityOnWorkflow":false,"hasManuscriptDocX":true,"hasOptedInToPreprint":true,"hasPassedJournalQc":"","hasAnyPriority":false,"hideJournal":false,"highlight":"","institution":"","isAcceptedByJournal":true,"isAuthorSuppliedPdf":false,"isDeskRejected":"","isHiddenFromSearch":false,"isInQc":false,"isInWorkflow":true,"isPdf":false,"isPdfUpToDate":true,"isWithdrawnOrRetracted":false,"journal":{"display":true,"email":"[email protected]","identity":"chemical-papers","isNatureJournal":false,"hasQc":true,"allowDirectSubmit":false,"externalIdentity":"chpa","sideBox":"Learn more about [Chemical Papers](http://link.springer.com/journal/11696)","snPcode":"11696","submissionUrl":"https://www.editorialmanager.com/CHPA/default.aspx","title":"Chemical Papers","twitterHandle":"","acdcEnabled":true,"dfaEnabled":true,"editorialSystem":"em","reportingPortfolio":"Springer Hybrid","inReviewEnabled":true,"inReviewRevisionsEnabled":false},"keywords":"Lithium-metal solid-state battery, Polymer blend matrix, Polymer composite ceramflux solid electrolyte, LLZO Ceramic Fillers","lastPublishedDoi":"10.21203/rs.3.rs-7606253/v1","lastPublishedDoiUrl":"https://doi.org/10.21203/rs.3.rs-7606253/v1","license":{"name":"CC BY 4.0","url":"https://creativecommons.org/licenses/by/4.0/"},"manuscriptAbstract":"\u003cp\u003eAdvancing lithium-metal solid-state batteries (LSSBs) demands innovative composite solid electrolytes with superior safety, energy density, and cycle life. Here, we report a high-performance polymer-ceramic composite solid electrolyte (PCCSE) engineered by integrating lithium perborate (LiBO\u003csub\u003e3\u003c/sub\u003e) and surface-functionalized lithium lanthanum zirconium oxide (LLZO) nanofibers into a polyethylene oxide/polyvinylidene fluoride (PEO/PVDF) matrix using an optimized Stokes\u0026rsquo; solution casting method. The synergistic interplay of LiBO\u003csub\u003e3\u003c/sub\u003e and LLZO disrupts polymer crystallinity, enhances amorphization, and facilitates ionic transport through robust polymer\u0026ndash;ceramic interfacial interactions. Advanced characterization via X-ray diffraction (XRD), Fourier-transform infrared spectroscopy (FTIR), ultraviolet\u0026ndash;visible spectroscopy (UV\u0026ndash;Vis), and electrochemical impedance spectroscopy (EIS) confirms reduced crystallinity, improved segmental chain mobility, and optimized ionic pathways. The resulting PCCSE achieves a remarkable ionic conductivity of 4.25 \u0026times; 10\u003csup\u003e\u0026minus;\u0026thinsp;5\u003c/sup\u003e S cm\u003csup\u003e-1\u003c/sup\u003e at room temperature and a wide electrochemical stability window of 5.33 V, enabling compatibility with high-voltage cathodes. Full-cell tests with a lithium metal anode and LiCoO₂ cathode demonstrate high specific capacity, exceptional rate capability, and 95% capacity retention after 100 cycles. The PCCSE effectively mitigates lithium dendrite growth through uniform ion conduction and enhanced interfacial stability. These findings position PCCSE as a promising, safe, and high-performance electrolyte for next-generation all-solid-state lithium-metal batteries, paving the way for scalable, high-energy-density energy storage solutions.\u003c/p\u003e","manuscriptTitle":"Polymer–Ceramic Framework Stabilized Solid Electrolyte for Advanced Lithium-Ion Energy Storage","msid":"","msnumber":"","nonDraftVersions":[{"code":1,"date":"2025-09-25 09:44:31","doi":"10.21203/rs.3.rs-7606253/v1","editorialEvents":[{"type":"communityComments","content":0},{"type":"decision","content":"Minor revisions","date":"2025-11-12T11:13:02+00:00","index":"","fulltext":""},{"type":"reviewerAgreed","content":"","date":"2025-09-22T07:13:42+00:00","index":0,"fulltext":""},{"type":"reviewersInvited","content":"","date":"2025-09-17T04:28:22+00:00","index":"","fulltext":""},{"type":"editorAssigned","content":"","date":"2025-09-16T12:04:42+00:00","index":"","fulltext":""},{"type":"submitted","content":"Chemical Papers","date":"2025-09-13T05:23:49+00:00","index":"","fulltext":""}],"status":"published","journal":{"display":true,"email":"[email protected]","identity":"chemical-papers","isNatureJournal":false,"hasQc":true,"allowDirectSubmit":false,"externalIdentity":"chpa","sideBox":"Learn more about [Chemical Papers](http://link.springer.com/journal/11696)","snPcode":"11696","submissionUrl":"https://www.editorialmanager.com/CHPA/default.aspx","title":"Chemical Papers","twitterHandle":"","acdcEnabled":true,"dfaEnabled":true,"editorialSystem":"em","reportingPortfolio":"Springer Hybrid","inReviewEnabled":true,"inReviewRevisionsEnabled":false}}],"origin":"","ownerIdentity":"c1abb5ae-54c5-451f-8103-3ed8f0d88a3b","owner":[],"postedDate":"September 25th, 2025","published":true,"recentEditorialEvents":[],"rejectedJournal":[],"revision":"","amendment":"","status":"published-in-journal","subjectAreas":[],"tags":[],"updatedAt":"2026-01-12T16:06:13+00:00","versionOfRecord":{"articleIdentity":"rs-7606253","link":"https://doi.org/10.1007/s11696-025-04605-4","journal":{"identity":"chemical-papers","isVorOnly":false,"title":"Chemical Papers"},"publishedOn":"2026-01-10 15:59:12","publishedOnDateReadable":"January 10th, 2026"},"versionCreatedAt":"2025-09-25 09:44:31","video":"","vorDoi":"10.1007/s11696-025-04605-4","vorDoiUrl":"https://doi.org/10.1007/s11696-025-04605-4","workflowStages":[]},"version":"v1","identity":"rs-7606253","journalConfig":"researchsquare"},"__N_SSP":true},"page":"/article/[identity]/[[...version]]","query":{"redirect":"/article/rs-7606253","identity":"rs-7606253","version":["v1"]},"buildId":"8U1c8b4HqxoKbykW_rLl7","isFallback":false,"isExperimentalCompile":false,"dynamicIds":[84888],"gssp":true,"scriptLoader":[]}

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