Role of Oxygen and Halogen Functionalization in Tuning the Surface Properties of Zr3C2T2 MXene for Lithium Storage: A Density Functional Theory Study

We constructed computational models of bare Zr<sub>3</sub>C<sub>2</sub> and surface-functionalized Zr<sub>3</sub>C<sub>2</sub>T<sub>2</sub> (T = O, S, F, Cl), and utilized first-principles calculations to systematically explore the effects of these surface-functionalized groups on the structural stability, electronic properties, and lithium storage performance of Zr<sub>3</sub>C<sub>2</sub>T<sub>2</sub>. Compared to halogen functional groups (e.g., F, Cl), the structure and electronic properties of Zr<sub>3</sub>C<sub>2</sub> are more profoundly influenced by oxygen group functional elements (O, S). The formation energy of Zr<sub>3</sub>C<sub>2</sub>T<sub>2</sub> (T = O, S) functionalized by the same periodic oxygen group elements is lower than that of Zr<sub>3</sub>C<sub>2</sub>T<sub>2</sub> (T = F, Cl) functionalized by the same periodic halogens. Regarding electronic properties, the oxygen and sulfur functional groups have strong hybridization with Zr<sub>3</sub>C<sub>2</sub> in the valence band and generate a new band structure, which makes the DOS move toward the conduction band. The adsorption energy calculations reveal that lithium ions exhibit stable adsorption on bare Zr<sub>3</sub>C<sub>2</sub> and O/S-functionalized Zr<sub>3</sub>C<sub>2</sub>T<sub>2</sub> surfaces, whereas no stable adsorption occurs on Zr<sub>3</sub>C<sub>2</sub>F<sub>2</sub> or Zr<sub>3</sub>C<sub>2</sub>Cl<sub>2</sub>. In terms of adsorbing lithium atoms, bare Zr<sub>3</sub>C<sub>2</sub> tends to adsorb at the HCP position, while Zr<sub>3</sub>C<sub>2</sub>O<sub>2</sub> and Zr<sub>3</sub>C<sub>2</sub>S<sub>2</sub> tend to adsorb at the CCP position. First-principles calculations indicate distinct theoretical lithium storage capacities for Zr<sub>3</sub>C<sub>2</sub>-based materials: monolayer adsorption yields capacities of 180.13 mAh/g (bare Zr<sub>3</sub>C<sub>2</sub>), 162.64 mAh/g (Zr<sub>3</sub>C<sub>2</sub>O<sub>2</sub>), and 148.20 mAh/g (Zr<sub>3</sub>C<sub>2</sub>S<sub>2</sub>); bilayer adsorption significantly increases these values to 360.25, 325.29, and 296.41 mAh/g, respectively.

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Journal
Materials
Published
2025-03-11
DOI
https://doi.org/10.3390/ma18061237
Citations
2
Primary Topic
MXene and MAX Phase Materials
Type
article
Field-Weighted Citation Impact
1.04

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article

Role of Oxygen and Halogen Functionalization in Tuning the Surface Properties of Zr3C2T2 MXene for Lithium Storage: A Density Functional Theory Study

Zhengyang Xie, Wenke Lu, Shouwei Wang, Yue Liu et al.
2 citations
Materials
MXene and MAX Phase Materials
1.04
article

Role of Oxygen and Halogen Functionalization in Tuning the Surface Properties of Zr3C2T2 MXene for Lithium Storage: A Density Functional Theory Study

Zhengyang Xie, Wenke Lu, Shouwei Wang, Yue Liu, Hui Li, Jinyi Liu, Tianwei Gao
article en
2 citations

Abstract

We constructed computational models of bare Zr<sub>3</sub>C<sub>2</sub> and surface-functionalized Zr<sub>3</sub>C<sub>2</sub>T<sub>2</sub> (T = O, S, F, Cl), and utilized first-principles calculations to systematically explore the effects of these surface-functionalized groups on the structural stability, electronic properties, and lithium storage performance of Zr<sub>3</sub>C<sub>2</sub>T<sub>2</sub>. Compared to halogen functional groups (e.g., F, Cl), the structure and electronic properties of Zr<sub>3</sub>C<sub>2</sub> are more profoundly influenced by oxygen group functional elements (O, S). The formation energy of Zr<sub>3</sub>C<sub>2</sub>T<sub>2</sub> (T = O, S) functionalized by the same periodic oxygen group elements is lower than that of Zr<sub>3</sub>C<sub>2</sub>T<sub>2</sub> (T = F, Cl) functionalized by the same periodic halogens. Regarding electronic properties, the oxygen and sulfur functional groups have strong hybridization with Zr<sub>3</sub>C<sub>2</sub> in the valence band and generate a new band structure, which makes the DOS move toward the conduction band. The adsorption energy calculations reveal that lithium ions exhibit stable adsorption on bare Zr<sub>3</sub>C<sub>2</sub> and O/S-functionalized Zr<sub>3</sub>C<sub>2</sub>T<sub>2</sub> surfaces, whereas no stable adsorption occurs on Zr<sub>3</sub>C<sub>2</sub>F<sub>2</sub> or Zr<sub>3</sub>C<sub>2</sub>Cl<sub>2</sub>. In terms of adsorbing lithium atoms, bare Zr<sub>3</sub>C<sub>2</sub> tends to adsorb at the HCP position, while Zr<sub>3</sub>C<sub>2</sub>O<sub>2</sub> and Zr<sub>3</sub>C<sub>2</sub>S<sub>2</sub> tend to adsorb at the CCP position. First-principles calculations indicate distinct theoretical lithium storage capacities for Zr<sub>3</sub>C<sub>2</sub>-based materials: monolayer adsorption yields capacities of 180.13 mAh/g (bare Zr<sub>3</sub>C<sub>2</sub>), 162.64 mAh/g (Zr<sub>3</sub>C<sub>2</sub>O<sub>2</sub>), and 148.20 mAh/g (Zr<sub>3</sub>C<sub>2</sub>S<sub>2</sub>); bilayer adsorption significantly increases these values to 360.25, 325.29, and 296.41 mAh/g, respectively.

MaterialsVol. 18(6)
Chang'an University (CN)
National College Students Innovation and Entrepreneurship Training Program
Affordable and clean energy
Openalex Percentile: Top 27%
MXene and MAX Phase Materials
1.04
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