Super Electrolyte-Philic Boron Nitride Nanotube Membranes as Highly Robust Separators for Lithium Batteries

The widespread deployment of lithium ion (Li + ) batteries with increasing energy density entails a worsening safety concern. Among many contributing factors, the typical polymer separators are plagued with poor thermal stability,limited mechanical strength and lower Li + transference number, and are prone to catastrophic failure when subjected to local thermalor mechanical stress (e.g., pierced by lithium dendrites). Herein, we report an all-inorganicnonwoven boron nitride nanotube membrane featuring exceptional chemical stability, thermal stability, re resistance and mechanical exibility. The resulting membranes show superior wettability to electrolyte to endow excellent Li + transport properties with the lowest ionic resistance and the highest Li + transference number (0.86) when compared with all commercial separators. They can thus function as highly robust separators for Li/Li symmetriccells with ultralow overpotential (8.5 mV) and exceptional reversibility for repeated lithium plating/stripping cycles for over 8000 hours, and for practical LiFePO 4 /Li cell with unusually high temperature stability. Our study denes a unique class of super electrolyte-philic ceramic separators with favorable mechanical strength, thermal stability and ion transfer properties for advanced lithium batteries. after chronoamperometry. h, Comparison of tLi+. i, j, XPS spectra of BNNTMs. N 1s (i), and Li 1s (j) high-resolution spectra. k, Raman spectra of BNNTMs before and after absorbing electrolyte (1 mol/L LiPF6 in 1:1 v/v EC/DMC with 2% VC) for 6 hours, and Raman spectra of electrolyte. l, Linear sweep voltammetry (LSV) (from 3 to 6 V) proles of Li/SS cells at a scanning speed of 1 mV s-1. The corresponding curves showing the electrochemical stability of the electrolyte with different separators at room temperature.

Extensive efforts have been made to improve the thermal stability and/or mechanical stability of the separators by coating surface of polyole n separators with inorganic nanostructures (e.g., SiO 2 , Al 2 O 3 , Al(OH) 3 , Mg(OH) 2 , Zeolite, ZrO 2 and TiO 2 ) 16,17,18,19,20 , incorporating inorganic llers (e.g., BN nanosheets or BN nanotubes) in polymer composites 5,21 , or introducing re-resistant moieties such as hydroxyapatite 22 , polyimide 23 and triphenyl phosphate 24 in the polymer backbones. These strategies can generally improve the ionic conductivity, reduce the local heat accumulation to prevent thermal runaway, while increasing the mechanical strength and re resistance to mitigate the risk of catastrophic failure.
Nonetheless, the overall robustness of these separators is fundamentally limited by the thermal stability and mechanical strength of the polymer matrix, and can still fail under large thermal gradients or extended high-temperature exposure. Additionally, these designs don't address the ionic transport limitations of typical polymer membranes 25,26,27 .
Herein, we report a new design of all inorganic ceramic separators based nonwoven boron nitride nanotube membranes (BNNTMs). The BNNTMs feature exceptional mechanical exibility and thermal stability to endure high mechanical or thermal stress, and at the same time exhibit superior electrolyte wettability, high ionic conductivity (2 mS cm −1 ) and high Li + ion transference number (0.86) to effectively minimize concentration polarization and suppress Li dendrite formation. They can thus function as highly robust separators for Li/Li symmetric cells with ultralow overpotential (8.5 mV) and exceptional reversibility for repeated lithium plating/stripping cycles for over 8,000 hours. Integrating BNNTMs with typical cathode and anode results in full batteries that with greatly enhanced rate capability. Furthermore, bene ting from its high thermal stability, the full batteries with BNNTMs can function well at high temperature up to 120 °C, opening a pathway to high-temperature batteries. Our study de nes a unique class of super electrolyte-philic ceramic separators with favorable mechanical strength, thermal stability and ion transfer properties for advanced LIBs. First, an electrospinning process was used to produce polypropylene cyanide (PAN) template followed by a high temperature carbonization process to produce nonwoven carbon bers mats (CNNT) with tunable porous structure. Next, a chemical vapor deposition (CVD) process was carried out to form BN layer on the surface of the carbon bers. Lastly, the carbon ber template was thermally etched to obtain BNNTMs. The template-synthesized BNNTMs clearly manifest typical interconnected anisotropic ber structures (Fig. 1b). High resolution scanning electron microscopy (SEM), transmission electron microscope (TEM) images demonstrate that the bers in the BNNTMs feature a hollow tubular structure with the wall thickness about 80 nm ( Fig. 1c and d). The corresponding energy dispersive X-ray (EDX) elementary mapping reveals uniform distribution of boron (B) and nitrogen (N) elements, with a small amount of oxygen (O) elements attributed to contamination in air during etch processes (Fig. 1e). The mechanical robustness under stress and deformation is a critical attribute of an ideal separator, which should withstand stress induced by local electrode volume change or lithium dendrite piercing 28 . To this end, the BNNTMs exhibit extraordinary mechanical exibility and strength, and can be fully folded and unfolded without affecting the structural integrity ( Fig. 1f-i).
To evaluate the potential of the BNNTMs as separators for practical LIBs, we compared a series of key structural and physical properties of the BNNTMs with commercial polypropylene (PP), cellulose ber (CF), ceramic (Ce), Lauren (La) separators. A summary of various physical properties of these separators are shown in Supplementary Table S1. Highly open and interconnected architecture is favorable for electrolyte stockpile and Li + diffusion, improving the rate capability and cycling stability of batteries 29 . To further evaluate the porous structure of separators, we conducted Gurley value and porosity test. A low Gurley value indicates fast air penetration through large pores or well-interconnected pores 30  The physical deformation (e.g., shrinkage) of the separators under thermal stress may lead to serious safety hazards 31,32 . Therefore, the thermal dimensional stability of the separators is critical for safe LIBs and dictates the highest temperature that the LIBs can operate. We have compared the thermal stability and ammability of the BNNTMs with commercial polyole n (PP, CF, Ce, La) separators. Fig. 2a shows the optical photographs of these different separators after thermal treatment at various temperatures from 100 to 800 °C in air for 30 min. Although all separators largely retain the original shape at 100 °C, the PP, Ce and La separators start to exhibit notable dimensional shrinkage and crispation at 150 °C and clearly decompose at 250 °C (color turns black). CF also deforms instantaneously at 250 °C and completely vaporizes at 300 °C. In contrast, the BNNTMs show extraordinary structure integrity up to 800°C , which is important for retaining the safety of the failing LIBs in which the local joule heating can exceed 200 °C 33 . The thermal stability of the separators at such high temperature can ensure structural integrity and prevent short circuiting, thermal runaway and catastrophic failure. Fig 2b compares the temperature at which large deformation occurs for each separator.
We have further conducted thermal gravity test and found that the BNNTMs show little weight loss up to 800 °C in air (Fig. 2b), con rming its excellent thermal stability. In contrast, all other commercial separators lost >70% of the total weight in the temperature regime of 300-400 °C, con rming serious chemical degradation at such temperature. Furthermore, the X-ray diffraction (XRD) analysis and Fourier transform infrared (FTIR) spectroscopy studies of the thermally stressed BNNTMs reveal that the major diffraction patterns and absorption peaks are well retained after thermal treatment ( Supplementary Fig.  3), further demonstrating the intrinsic material stability of the BNNTMs.
We have further conducted ammability test. The PP and CF are immediately melted and burned out upon contacting with flame, and the Ce and La are also easily ignited and combusted ( Supplementary  Fig. 4). With extraordinary thermal stability and chemical inertness, the BNNTMs show no obvious structural change in ame, demonstrating outstanding incombustibility with signi cant potential as ame-resistant separators.
Change of pore size in commercial polyole n separators under thermal stress may degrade the cycling performance or cause serious safety issues 34 . The SEM images of the separators after annealing at 150 for 1 h are shown in Figure 2c-l. In general, the oriented elliptical pores notably shrink and turn to round in PP separator due softening and shrinking of PP under thermal stress. Similar pore shrinkages are also observed in for Ce and La membranes, whereas the CF and BNNTMs largely maintain homogeneous interconnected porous architecture.
Ion transport properties across the separators are mostly governed by the wettability of the electrolytes 35 .
The high electrolyte uptake ability of the separators is essential for high ionic conductivity 30 . We have therefore evaluated electrolyte wetting behavior of different separators by conducting the contact angle measurements and evaluating the wetted area as a function of the contacting time (Fig. 3a). The wettability depends upon a number of factors, including intrinsic molecular interactions, porosity, and surface roughness. A small droplet of electrolyte on the PP separator shows little change after 60 s of contact, indicating a poor wettability, which can be attributed to the low surface energy and nonpolar nature of PP 6 . Ce and La exhibit better wettability than PP owing to their polar Al-OH groups of Al 2 O 3 particles and polar -NH 2 groups of benzoyl diamine on the coating layer. The CF and BNNTMs demonstrate excellent a nity to the electrolytes. In particular, the electrolyte is instantly absorbed into BNNTMs upon in contact, which exhibits essentially zero degree of contact angle ( 106%) after the immersion in the liquid electrolyte for 3 h. The excellent wettability and electrolyte uptake characters may be attributed to the polar B-N bonds that have favorable interaction with the electrolyte (to be further discussed later) and the 3D interwoven porous architectures that further enhance the wettability endow super electrolyte-philic characteristics 36,37 . Such a superior wettability promises high ion conductivity to ensure the uniformity of Li ion flux and mitigates uneven Li ion transport, deposition and lament formation.
We have next evaluated the ion transport properties across the BNNTMs by conducting electrochemical impedance spectroscopy (EIS) studies. Expectedly, the BNNTMs show the highest ionic conductivity (2.00 mS cm -1 ) at 25 °C ( Fig. 3c and Supplementary Fig. 6), which is about 7.2, 1.5, 3.9 and 2.1 times of those of PP (0.28 mS cm -1 ), CF (1.33 mS cm -1 ), Ce (0.51 mS cm -1 ), La (0.95 mS cm -1 ). Fig. 3d shows Nyquist plots for BNNTMs at different temperature and the corresponding impedance values (horizontal X-axis intersects) (see the Supplementary Fig. 7 for Nyquist plots and corresponding impedance values for commercial separators). Fig. 3e exhibits corresponding Arrhenius plots of ionic conductivity (ơ) and Linear tting results for different separators. It is clear that the ionic conductivity of the BNNTMs is higher at all temperature. Additionally, the BNNTMs show the lowest activation energy (E a ) of 0.08 eV for ion transport, compared to 0.10-0.28 eV for other separators (Fig. 3f), which is expected to reduce the Ohmic polarization and therefore enhance the electrochemical performance of batteries.
Lithium-ion transference number (t Li + ) is a critical parameter when evaluating the ionic conductivity for Liion batteries. Low t Li + gives rise to concentration polarization, leading to side reactions, dendrite growth and joule heating, which can shorten cycling life and cause catastrophic failure especially under fast charging/discharging condition 38,39 . It is thus important to determine the extract t Li + . Our measurements give a t Li + of 0.86 for the BNNTMs, which is considerably higher than those of the other commercial separators (0.37-0.69) (Fig. 3g, h and Supplementary Fig. 8). The simulated equivalent circuit and the AC impedance spectra results of symmetrical battery are shown in Supplementary Table S2.
Such improvement could be interpreted from two aspects. On one hand, the BNNTMs own high porosity, excellent wettability and uptake to the liquid electrolyte. On the other hand, BN may act as both a Lewis base and acid. Li ions may directly interact with nitrogen (Lewis base) in BN instead of intensely solvated by solvent molecules before deposition, and thus speed up the dissociation of Li ions and lithium salt. Xray photoelectron spectroscopy (XPS) was performed to investigate interactions of the BNNTMs toward cm -1 (Figure 3k and Supplementary Fig. 9). The BNNTMs show no peaks in the region of 100-1000 cm -1 .
Whereas, after absorbing electrolyte, the BNNTMs show resonance peaks with different positions and intensities from those of the electrolyte itself, indicating strong interactions between the BNNTMs and the electrolyte. To further con rm anion-trapping ability of the BNNTMs, TFSIvibration was monitored to analyzing the Li + coordination state with TFSIanion. It could be divided into two components: free TFSI -(742 cm -1 ) and Li + coordinated TFSIanions (748 cm -1 ) 41 . Supplementary Fig. 10 clearly shows that BNNTMs demonstrate a larger content of dissociated Li + ions through immobilization of TFSIanion than other separators. Therefore, the BNNTMs exhibit much improved t Li + . Being both a Lewis acid and base, the BNNTMs show favorable interaction with both the cations and anions, leading to superior wettability, and combining its highly porous structure, the BNNTMs show much desired super electrolyte philicity.
Lastly, we have further evaluated the enhanced electrochemical stability of the BNNTMs by conducting linear sweep voltammetry (LSV) (Fig. 3l). In general, with the commercial separators, the LSV show a notable the current density increases at potentials above 4.3 V, indicating the onset of electrolyte decomposition. Signi cantly, no current increase is observed with the BNNTMs until a much higher potential of ~5.3 V, suggesting a much higher decomposition potential and wider electrochemical window. The improved stability is an interesting topic for further studies, which might be partly attributed to the strong interactions between the BN with anions, which may help lower the extent of anion oxidation at a high potential 42,43 , thus alleviating the decomposition of the carbonate electrolytes and promoting the kinetics of electrode reactions, generating a more stable interface between the electrolyte and the electrode. The wider electrochemical stable window would open opportunities for high-voltage LIBs.

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The formation of Li dendrites during repeated cycling is a common challenge in lithium metal batteries.
Such dendrite formation can be largely attributed to ine cient Li + transport that leads to concentration polarization and uneven charge distribution 38 . It is important in controlling Li dendrite formation by alleviating the anion depletion-induced large electric elds near the Li anode. Based on their excellent electrolyte wettability and Li + transport properties, we have explored the BNNTMs as the separators for Li metal electrodes. Fig. 4a shows the cycle performance and voltage hysteresis of the Li symmetric cells at a current density of 1 mA cm -2 . With the BNNTMs as the separator, the galvanostatic plating/stripping pro le shows highly stable electrochemical process with little potential undulation. In contrast, the overpotential gradually increases upon cycling for CF, and violently uctuates after 230 h, which may be  Fig. 11). In contrast, the device with BNNTMs shows stable voltage pro les with an ultra-small overpotential (8.5 mV) beyond 6,500 h, which remains 2 0 mV after 8,000 h continuous operation.
When the high current density of 3.5 mA cm -2 is applied, concentration polarization starts to increase. Uneven current distribution and Li deposition may result in increasing overpotential during cycles. For example, the commercial separators show a much large overpotential up to ~ 500 mV with large voltage uctuations. Nonetheless, the device with the BNNTMs still exhibits outstanding stability for more than 700 h with a stable overpotential of 12 mV (Fig. 4b, and inset)).
We have further compared the photographs and SEM images of fresh Li foil and Li electrode after 340 mAh cm -2 cumulative capacity at 1 mA cm -2 to evaluate the lithium metal surface morphology change over cycling (Fig. 4c-h and Supplementary Fig. 12). Before cycling, the fresh Li foil exhibits metal luster with relatively at surface. After cycling with different commercial separators, the Li foils show apparent blackening trend. By contrast, the metal luster is largely retained in Li foil cycled with BNNTMs. The SEM images of the fresh Li foil show relatively at surface, while those of Li foils cycled with commercial separators show considerable surface roughness and inhomogeneity due to Li dendrite formation. On the other hand, the SEM image of Li foil cycled with BNNTMs show relatively smooth surface largely comparable to the fresh foil, indicating little dendrite formation. Signi cantly, the metal luster and relatively smooth surface are also largely retained in device with BNNTMs after cycling at 3.5 mA cm -2 ( Fig. 4i), demonstrating little dendrite formation even under high current density.
The long-term stability and well-controlled Li deposition endowed by BNNTMs are originated from the collective effect of its favorable interactions with electrolyte to unify Li + ux. As compared with results across the published reports, the devices with the BNNTMs separator exhibit excellent Li dendritesuppressing ability to enable exceptional small overpotential (Supplementary Fig. 13) and cycling stability with a cumulative lifetime capacity exceeding 4,000 mAh cm -2 , exceeding the lifetime capacity of typical LIBs (typically < 2,000 mAh cm -2 ) 44,45,46,47,48,49,50,51,52,53,54,55,56,57,58,59,60 (Fig. 4j)  To assess the practical applicability of the BNNTMs in LIBs, we have also used the BNNTMs separators for LiNi 0.5 Co 0.2 Mn 0.3 O 2 (NCM523)/graphite coin cells and compared the electrochemical performance of the same cells with commercial separators. Stepped rate performance tests were carried out from 0.1 to 5 C and then back to 1 C. Fig. 5a shows charge-discharge voltage pro les of 1 st cycle for NCM/graphite cells. Supplementary Fig. 14 displays the typical charge-discharge voltage pro les of full cells at different rates. Overall, the cell with BNNTMs delivers much better rate capability and manifests discharge capacities of 308.7, 278.8, 259.7, 215.5, 185.9, 136.8 and 97.8 mAh g -1 at various rates 0.1 C, 0.5 C, 1 C, 2 C, 3 C, 4 C and 5 C, respectively (Fig. 5b). In contrast, the device with commercial separators (PP, Ce, La) fails to deliver meaningful capacity at 3 C.
To further verify the excellent thermal stability of the BNNTMs separators, we evaluated the cycling performance of LiFePO 4 /Li cell with various separators at 1 C by using commercial liquid electrolyte (LX-0081) at 120 °C. Clearly, The LiFePO 4 /BNNTM/Li cell shows stable voltage pro les and a gravimetric discharge capacity of 151.8 mAh g -1 with a CE of 99.99% at 120 ℃ (Figure 5c) and exhibits a relatively high gravimetric discharge capacity retention of 83%, while the cells with commercial separators stop running after several cycles ( Supplementary Fig. 15). These results indicate that the BNNTMs separators can offer signi cant potentials for high temperature LIBs. It should also be noted that 120 ℃ operating temperature demonstrated here is not limited by the BNNTMs separators, buy by the electrode materials or electrolyte used.
In summary, we have reported a unique design of all-inorganic BNNTMs separators with exceptional chemical stability, thermal stability, re resistance and mechanical exibility. The BNNTMs feature super electrolyte philicity to endow excellent Li + transport properties with the lowest ionic resistance and the highest Li + transference number compared with all commercial separators, making them highly robust separators for Li metal battery. Moreover, the BNNTMs separators exhibit better rate and cycling durability at room and 120 ℃. Our study de nes a unique class of super electrolyte-philic ceramic separators for advanced LIBs. Other characterization techniques. The samples were characterized by scanning electron microscopy (SEM) images and electron dispersive X-ray spectroscopy (EDS) mappings of the samples were obtained on a SIGMA microscope (Zeiss, Germany) equipped with an EDS spectrometer. Transmission electron microscopy images and X-ray diffraction (XRD) patterns were obtained on a JEM-2100F microscope (JEOL, Japan), a XRD-6100 spectrometer with Cu-Kα radiation (Shimadzu, Japan). The thermotropic behavior was tested using Thermo Gravimetric Analyzer (TGA, model TGAQ 50,      Lithium plating/stripping performance of BNNTMs separators. a, b, Galvanostatic plating/stripping pro les of Li / Li symmetric cells with different separators at low current density of 1 mA cm-2 with 2 mAh cm-2 cycling capacity (a) and at high current density of 3.5 mA cm-2 with 2.8 mAh cm-2 cycling capacity (b). The individual gures are stripping and plating curves at different states. c-i, The corresponding SEM of Li foil. Fresh (c) and after cycling 340 mAh cm-2 cumulative capacity for different separators at 1 mA cm-2 (d-h) and after 476 mAh cm-2 cumulative capacity for BNNTMs at 3.5 mA cm-2 (i), respectively. j, Comparison of plating/stripping cumulative capacity in Li/Li symmetric cells with existing papers.

Figure 5
Electrochemical performance of NCM/graphite full cells and LiFePO4/Li cells using different separators.
a, Corresponding galvanostatic charge-discharge voltage pro les for NCM/graphite full cells at 1 C (1st cycle). b, Rate performance of different separators for NCM/graphite full cells. c, Cycling performances of LiFePO4/Li cell with BNNTMs at 1 C at 120 °C.