First-principles insights into selenium and sulfur doping on Ti<sub>2</sub>CO<sub>2</sub> MXene for mitigating the shuttle effect in lithium–sulfur batteries
Abstract Lithium–sulfur (Li–S) batteries are promising next-generation energy storage devices due to their high energy density, cost-effectiveness, and environmental friendliness. However, their practical application is hindered by the shuttle effect of lithium polysulfides (Li 2 S x ) and the poor electrical conductivity of the sulfur cathode. In this study, we employ first-principles density functional theory calculations to investigate the effects of selenium (Se) or sulfur (S) doping on Ti 2 CO 2 MXene as an anchoring material to mitigate these challenges. Our findings reveal that substituting oxygen with Se or S enhances the electronic conductivity of Ti 2 CO 2 by transforming it into a metallic conductor. The adsorption energies of various Li 2 S x clusters ( x = 1, 2, 4, 6, 8) on the doped MXenes demonstrate significantly improved binding, particularly for low-sulfur content clusters, which is crucial for inhibiting the shuttle effect. Furthermore, charge transfer analysis confirms that Se or S doping enhances the interaction between Li 2 S x and the MXene surface, promoting better electrochemical performance. These results establish Se or S doping as an effective strategy for optimizing MXene-based anchoring materials in high-performance Li–S batteries.
Authors
- Minh Triết Đặng (ORCID: https://orcid.org/0000-0003-1769-4873)
- Nguyen Thi Bao Trang (ORCID: https://orcid.org/0009-0003-1518-8333)
- Nguyen Truong Long (ORCID: https://orcid.org/0000-0002-6127-254X)
- Anh Duy Nguyen Vo
- Thu Hoa Nguyen Thi
Institutions
- Hanoi Architectural University (VN)
- Can Tho University (VN)
Publication Details
- Journal
- Advances in Natural Sciences Nanoscience and Nanotechnology
- Published
- 2025-09-25
- DOI
- https://doi.org/10.1088/2043-6262/ae0b6f
- Citations
- 1
- Primary Topic
- MXene and MAX Phase Materials
- Type
- article
- Field-Weighted Citation Impact
- 0.52