Solid-state lithium (Li) batteries are hailed as the next-generation energy storage technology, garnering significant attention for their potential high energy density and safety. Particularly when using Li-rich manganese layered oxide (LRMO) as cathodes (theoretical capacity exceeding 250 mAh/g), energy densities over 600 Wh/kg can be theoretically achieved [
1,
2]. However, reality often falls short of such ideals. Solid-state batteries face significant interfacial challenges in practical applications. The core issues include high interfacial impedance from poor solid-solid contact and the instability of electrolytes against both high-voltage cathodes (above 4.5 V) and strongly reductive anodes [
3,
4]. For example, conventional polyether (PE)-based electrolytes undergo oxidative decomposition at voltages exceeding 4.0 V, triggering persistent interfacial side reactions. This incompatibility is further exacerbated in LRMO cathodes under high voltages, where irreversible oxygen-involved redox reactions occur, leading to oxygen loss, structural degradation, and severe electrolyte decomposition. Concurrently, the poor oxidation resistance and insufficient Li-ion transport kinetics of conventional PE electrolytes accelerate battery failure. Although applying high external pressure and designing multi-layer electrolytes were shown to improve interfacial contact, these methods introduce practical complications. Sustaining high pressure is difficult, and complex structures often create new interfacial resistances, layer-matching issues, and impaired ion transport. Therefore, the key scientific challenge for practical solid-state batteries lies in constructing stable and efficient solid-solid interfaces without resorting to high external pressure or structural complexity.
In a recent
Nature paper, Zhang, Zhao, and colleagues proposed an innovative “anion-rich solvation structure” design strategy for solid-state batteries within the key principles of Li-bond chemistry (
Fig. 1a) [
5]. Through precise molecular design, a series of in-built solid polymer electrolytes (SPEs) were obtained
via thermally initiated
in-situ copolymerization of a strongly solvating PE monomer (poly(ethylene glycol) methyl ether acrylate) with weakly solvating fluorohydrocarbon monomers of varying side-chain lengths. Among them, the PTF-PE copolymer, incorporating the longest fluorohydrocarbon monomer of 2,2,3,3,4,4,5,5,6,6,7,7-dodecafluoroheptyl acrylate, exhibits optimal thermal and oxidation stability. Upon incorporation of Li salt, a unique “−F⋯Li
+⋯O−” three-center coordination structure forms induced by intermolecular Li bonding. 2D
1H−
1H NOESY nuclear magnetic resonance (NMR) spectra of PTF-PE-salt reveal strong cross-peaks that are absent in the copolymer, confirming a close proximity (< 10 Å) between PTF and PE chains induced by Li
+ (
Fig. 1b). Complementary
1H and
19F solid-state NMR spectra further validate the direct interaction between Li
+ and –CF
2 fluorine atoms. Such an interaction upon chain proximity is verified by density functional theory (DFT) calculations, and the F···Li
+ bond formation is shown to weaken the initially strong interaction between Li
+ and PE chains (
Fig. 1c). Thus, the unique coordination structure regulates the Li
+ solvation microenvironment, facilitating Li
+ dissociation from polymer chains and promoting anion participation in contact ion pairs and aggregates, thereby shifting the solvation structure from “solvent-rich” to “anion-rich”. This Li-bond-based distinct solvation structure drives the spontaneous formation of uniform, stable F-rich interphases at both electrodes, simultaneously suppressing lattice oxygen escape and side reactions at the cathode and guiding uniform Li deposition at the anode. Moreover, with the strongly electron-withdrawing fluorinated groups, the oxidation stability of SPEs is significantly enhanced, resulting in widened voltage window to 4.7 V. Through above Li-bond-motivated dual-interfacial stabilization strategies, this electrolyte system successfully resolves the compatibility issues between high-voltage cathodes and highly reductive anodes in solid-state batteries.
Based on the innovative electrolyte structure and interface regulation strategy, LRMO-based solid-state Li metal batteries using PTF-PE-SPE demonstrate outstanding electrochemical performance. Specifically, after 500 cycles at a 1.0 C rate, the Li|PTF-PE-SPE|LRMO cell retains 72.1% of its capacity with an average coulombic efficiency of 99.5% (
Fig. 1d). More notably, a 9-Ah anode-free pouch cell (Cu|PTF-PE-SPE|LRMO) achieves a gravimetric energy density of 604 Wh/kg and a volumetric energy density of 1027 Wh/L under low external pressure of only 1 MPa, substantially exceeding commercial Li iron phosphate batteries (150–190 Wh/kg) and Li nickel cobalt manganese oxide batteries (240–320 Wh/kg) (
Fig. 1e). This achievement places its specific energy far above the reported state-of-the-art Li metal pouch cells with polymer or inorganic electrolytes, illustrating the extraordinary effectiveness of PTF-PE-SPE in practical Li batteries. Another significant breakthrough of this work lies in successfully resolving the inherent trade-off between high energy density and safety. Experimental results confirm that even in the fully charged state, the Li|PTF-PE-SPE|LRMO pouch cell passes both nail penetration and 120 ℃ thermal box tests without combustion or explosion. EV-ARC data reveals a thermal runaway temperature of 216.0 ℃, significantly higher than the 122.6 ℃ threshold for liquid electrolyte batteries, demonstrating intrinsic safety characteristics (
Fig. 1f). By enhancing the insulating layer and separator through PTF-PE-SPE technology, potential damage during thermal runaway in LRMO-based Li metal batteries can be effectively mitigated.