Meng-Ting Li*ab,
Jun Chena,
Ke Rena,
Xian-Hong Lia,
Hai-Yang Gaoa,
Da-Qiang Sunb and
Yang Yu*a
aCollege of Chemistry and Chemical Engineering, Qufu Normal University, Qufu, 273165, People's Republic of China. E-mail: limt0205@qfnu.edu.cn
bShandong Sacred Sun Power Sources Co., Ltd, No. 1, Shengyang Road, Qufu, Shandong 273100, China
First published on 15th December 2022
To address the problem of shutting effect of Li–S batteries, we used Ti-based MOF as precursor to obtain a conductive matrix with dual inhibitors. The target material, namely NTiPC, shown remarkable discharge capacity with 1178 mA h g−1, and maintained at 732 mA h g−1 after 100 cycles. The results indicated the N- and Ti-active sites synergistic acted with conductive framework can facilitate binding reaction between matrix and polysulfides.
Instead of adopting active sites (N- or TMOs) doped porous carbon materials as the host of sulfur followed by traditional synthesis method, the use of metal–organic frameworks (MOFs) with ordered crystalline structures as precursor have been certified to make framework structures and active elements distribute more uniformly, improve sulfur utilization and facilitate the kinetics of the Li–S redox reaction.19,20 MOFs, with metallic centers and redox active organic linkers, is already proven to be used in the field of electrode materials.21,22 As ideal host materials, MOFs with long range ordered channels to fabricate cathode composites can confine the polysulfides species through the confinement effect.23,24 Nevertheless, the inherent insulating properties of crystalline MOFs limit their electrochemical performance as host for sulphur.25 Hence, modulating the conductivity of MOFs while inheriting part of its structural and physicochemical characteristics is an effective way to adjust the host of sulfur.
Based on these, we attempted to use a nitrogen- and titanium-codoped porous carbon nanocomposites, which derived from Ti-based MOFs, as host to accommodate large amounts of sulfur. By using this Ti-assisted N-inhibiting strategy, nitrogen and titanium-doped porous carbon exhibiting incredible reversible charge/discharge performance, capacity retention ability and high electronic conductivity.
Brunauer–Emmett–Teller (BET) specific surface area of as-prepared TiPC and NTiPC are 546 and 414 m2 g−1 respectively (Fig. S2†). A considerable decrease in BET surface area for NH2-MIL-125(Ti) was caused by the presence of amine groups inside of the matrix. However, the specific surface area of S/TiPC and S/NTiPC are only 12 and 13 m2 g−1, which is demonstrated the successfully encapsulated of sulfur. Therefore, the sufficient sulfur loading could be ensured. The isotherms exhibit types I sorption behaviour typical for microporous materials. Both TiPC and NTiPC have average pore size of approximately 5 nm.
According to TGA (Fig. S3†), all of the as-synthesized and prepared materials possess approximately 50 wt% loading quantitative of sulfur. Based on the reported by Fu et al., the main weight loss of MIL-125(Ti) and NH2-MIL-125(Ti) are higher than 300 °C,32 so the pretreatment samples without solvent molecules were tested at the thermal weight loss range of sulfur. XRD patterns further demonstrated the successfully loading of sulfur. The experimental diffraction pattern of S/MIL-125(Ti) and S/NH2-MIL-125(Ti) are obeyed with the Ti-based MOFs. It means that the structural integrity is maintained in time of sulfur encapsulation procedure. In addition, TiPC and NTiPC show amorphous carbon materials pattern, and diffraction peaks of sulfur appear in S/TiPC and S/NTiPC, which confirmed the successful loading of sulfur (Fig. S1†).
Scanning electron microscopy (SEM) morphologies show the images of Ti-based MOFs, TiPC, NTiPC, S/TiPC and S/NTiPC as shown in Fig. 2 and S4.† The synthesized MIL-125(Ti) exhibit well-defined disk-like morphology, and the NH2-MIL-125(Ti) play a square piece morphology. After calcination, TiPC and NTiPC inherit the shape of precursors. There is no obvious sulfur aggregation but a highly dispersed state on the surface of the samples. This phenomenon is usually unavoidable in one-step homologous thermal decomposition.33–35
Fig. 2 SEM images of NH2-MIL-125(Ti) (a), NTiPC (b) and S/NTiPC (c), respectively. The elemental mapping of carbon (d), nitrogen (e), oxygen (f), titanium (g) and sulfur (h) of S/NTiPC. |
The distribution of different elements in the S/TiPC and S/NTiPC is investigated by energy-dispersive X-ray (EDX) spectroscopy mapping analysis. The uniform distributions of N and Ti elements suggest that the NTiPC matrix are formed in almost all particles. The strong EDX signal of sulfur in these composites imply the large amount of sulfur in the final cathodes. The XPS survey spectra reveals the surface chemical composition and functional groups of the NTiPC and S/NTiPC composites. The result shows that the presence of N-, C-, O-, S- and Ti-related peaks in the survey spectra (Fig. 3a). The peaks at 164 and 228 eV for S/NTiPC are attributed to S 2p and S 2s, respectively. The doublet peaks observed at 458.8 and 464.4 eV in NTiPC, and the peaks at 458.9 and 464.5 eV in S/NTiPC were characteristic of the TiO2 species (Fig. 3b). Another minor feature located at 457.4 eV in both NTiPC and S/NTiPC was attributed to a Ti2O3 surface phase. The there peaks at 400.5 eV, 396.9 eV and 395.9 eV in the N 1s spectrum of NTiPC (Fig. 3c) indicated the presence of quaternary N, pyrrolic N and pyridinic N species, respectively. The peaks at 401.5 eV, 398.8 eV and 396.3 eV in the N 1s spectrum of S/NTiPC are in the same circumstance. The N- and Ti-doped dual active sites are considered to enhance the binding strength and energy of the nonpolar atoms of host with polar polysulphides of guest, thus significantly increasing the long-cycle stability.
To investigated the electrochemical behavior of TiPC and NTiPC, we adopted a series of contrast materials to eliminate other factors. Such as anatase TiO2, unprocessed carbon and as-prepared Ti-MOFs precursor. Cyclic voltammetry (CV) analysis was used to prove the discharge/charge cycling performance and the presence of active substances of sulphur in a half cell. As shown in Fig. 4, all of the cathode materials showed obvious characteristic redox peaks of Li–S batteries, which is the working voltage range of the cells cycled at low rates. The characteristic reduction peaks at 2.3 V and 2.0 V are belonging to the multistep reduction of sulfur with Li.36,37 The oxidation peak approximately 2.4 V vested in reaction behaviour. The oxidation peak of S/MIL-125(Ti) and S/NH2-MIL-125(Ti) cathodes accompanies a broad peak starting at 2.3 V to 2.6 V, which is believed to be a feature of the active material within confined structures.38 Notably, the peaks of S/NTiPC at 5th cycle matches well with the initial ones without barely position offset or dramatically intensity decrease. Thus, NTiPC as host, possesses excellent electrochemical stability which attributed to the Ti-assisted N-inhibiting strategy and confinement effect of derivative framework. SEM images indicate that the morphology of NTiPC remained stable after several cycles of discharge/charge cycling (Fig. S5†).
Fig. 4 CV curves of in a range of S/MIL-125(Ti), S/TiPC, S/NH2-MIL-125(Ti) and S/NTiPC cathodes 1.5–3 V with a scanning rate of 0.1 mV s−1. |
Nyquist profiles of AC impedance represent the dynamics performance of batteries (Fig. S6†). The charge transfers resistance (Rct) of S/MIL-125(Ti), S/TiPC, S/NH2-MIL-125(Ti) and S/NTiPC cathodes at the first cycle are 70.1 Ω cm−2, 38.8 Ω cm−2, 259.9 Ω cm−2, 112.7 Ω cm−2, 99.3 Ω cm−2, 28.5 Ω cm−2, respectively. The Rct of NTiPC and S/NTiPC cathodes are almost the same, which lower than other cathodes materials and have better electrical conductivity. Obviosity, the Rct value is higher when micro crystalline Ti-MOFs used as anode materials directly. After high-temperature carbonization, NTiPC derived from Ti-MOFs can reduce the resistance of electron transfer and bring out lowest Rct value. Furthermore, the N- and Ti-active sites synergistic acted with conductive matrix can facilitate the electrolyte infiltration, which has triggered the easily interface ion transfer and leaded to a lower Rct.
When evaluated as cathode of Li–S batteries, NTiPC nanocomposite exhibits excellent discharge/charge capacity and cycling performance at 0.5 C-rate (1C = 1672 mA h g−1) in the voltage window of 1.5–3 V (Fig. 5). The capacity decay of S/TiO2 is dramatically, even though it possesses the highest discharge capacity of 1271 mA h g−1 at 1st cycle (Fig. S7†). It can only be maintained at approximately 510 mA h g−1 after 40 cycles. The discharge capacity of battery with the S/carbon cathode is at most 636.9 mA h g−1, but its capacity retention ability is good.
Fig. 5 Discharge/charge curves of the S/MIL-125(Ti), S/TiPC, S/NH2-MIL-125(Ti) and S/NTiPC cathodes at different cycles at 0.5C. |
The discharge capacities of S/MIL-125(Ti), S/TiPC, S/NH2-MIL-125(Ti) and S/NTiPC cathodes at 1st cycle is 568, 928, 800 and 1178 mA h g−1, respectively. By contrast, S/NH2-MIL-125(Ti) cathode has higher discharge capacity and retention rate to S/MIL-125(Ti), which provides N-active sites are favourable inhibitor of polysulfide shuttle. The contrast between microcrystalline MIL-125 and TiPC derivatives is well illustrated that the TiO2 as active sites could be uniformly dispersed in the conductive matrix after carbonization. And that makes a lot of sense why the S/NTiPC cathode exhibited a remarkable discharge capacity and a proper capacity retention ratio. After 40 cycles the capacity of S/NTiPC cathode as high as 912 mA h g−1.
After 100 cycles, the capacity of S/NTiPC cathode still stands at 732 mA h g−1 with nearly 100% coulombic efficiency, which is extremely better than that S/TiPC cathode with value of 456 mA h g−1 (Fig. 6). The capacity of S/TiO2 and S/carbon remain to be only 376 and 472 mA h g−1 after long discharge/charge process, demonstrating the derivative matrix with N- and Ti-codoped sites is the main contributor to the overall capacity. In addition, while S/NH2-MIL-125(Ti) can maintain at 445 mA h g−1, and S/MIL-125(Ti) can only maintain at 358 mA h g−1. It means that co-doped strategy is double insurance for capacities retention. Cycling performance at higher rate is necessary to evaluate. The experimental results show that the discharge capacity of the battery decreases obviously with the increase of current density, especially at higher rate, and the capacity retention rate is only about 50% (Fig. S8†). When the sulfur doping mass ratio of the NTiPC (at 900 °C for 2 h) is 1:3, the initial discharge capacity is more than 1600 mA h g−1. But the decay rate is very fast, and the capacity retention rate is only 25% (Fig. S9†). It is due to the overloading of sulfur, which causes most of the sulfur to simply adhere to the surface of the material, rather than in the pores. Under the same sulfur-carrying mass ratio and carbonization temperature condition, when the carbonization time increases, the cyclic stability of the material is improved, but the specific discharge capacity decreases sharply. We speculate that the reason for this phenomenon is that the carbonization of the material for a long time leads to the aggregation of the active sites within the material, which cannot effectively inhibit the shuttle of polysulfides. In addition, if the carbonization temperature of the material is lower than 900 °C, the specific discharge capacity of S/NTiPC cathode is also relatively low.
Fig. 6 The discharge capacity of S/MIL-125(Ti), S/TiPC, S/NH2-MIL-125(Ti) and S/NTiPC cathodes and the coulombic efficiency of S/NTiPC cathode at 0.5C during 100 cycles. |
The rate cycling capabilities of these cathodes are investigated at different current density from 0.2 to 1C (Fig. S10†). The average capacities of S/NTiPC are 1350, 1007, 832 and 689 mA h g−1 at 0.2C, 0.5C, 0.8C and 1C rates respectively, indicating a high charge/discharge capability. When the current density was resettled to 0.2C, S/NTiPC can be resumed to 989 mA h g−1, that the structure of NTiPC still stable after suffering high current density test. In comparison, the average discharge capacities for S/TiPC at different rates are 700, 507, and 397 mA h g−1, and capacities for S/MIL-125(Ti) are 566, 421, 382 and 356 mA h g−1, and capacities for S/NH2-MIL-125(Ti) are 901, 655, 563 and 494 mA h g−1 respectively. In short, by using N- and Ti-active sites as dual-inhibitors, NTiPC can effectively mitigate the polysulfides shuttle effects.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d2ra06372g |
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