High-Energy-Density Cathode Material Achieved by Upgrading Low-Voltage Li<sub>3</sub>V<sub>2</sub>O<sub>5</sub> via Ni Doping

High-energy-density lithium-ion batteries have great need for cathode materials with exceptional specific discharge capacity. Li<sub>3</sub>V<sub>2</sub>O<sub>5</sub> shows great potential because of its high capacity (e.g., 266 mA h g<sup>-1</sup> at 0.1 A g<sup>-1</sup>). However, its low-lying voltage plateau (∼0.6 V vs Li<sup>+</sup>/Li) restricts its use exclusively to anode applications. This work presents for the first time the development of Li<sub>3</sub>V<sub>2</sub>O<sub>5</sub> as a high-energy-density cathode material through Ni doping. Structural analysis reveals that Ni-doped Li<sub>3</sub>V<sub>2</sub>O<sub>5</sub> forms a cation-disordered rock-salt phase with a uniform distribution of Ni. Introducing 1 mol % Ni (denoted as LVON2) prolongs the V-based plateau (∼2.5 V) and results in an additional discharge capacity of 35 mA h g<sup>-1</sup>. In particular, a plateau ascribed to Ni<sup>2+</sup>/Ni<sup>3+</sup> redox reaction emerges at ∼3.5 V, contributing an extra discharge capacity of 42 mA h g<sup>-1</sup>. Consequently, LVON2 achieves high specific discharge capacities of 270.8 mA h g<sup>-1</sup> at 50 mA g<sup>-1</sup> and 339.4 mA h g<sup>-1</sup> at 20 mA g<sup>-1</sup> (corresponding to an energy density of 837 W h kg<sup>-1</sup>), surpassing the pristine Li<sub>3</sub>V<sub>2</sub>O<sub>5</sub> and many latest cathode materials. Density functional theory calculation shows that Ni preferentially occupies the empty tetragonal sites in Li<sub>3</sub>V<sub>2</sub>O<sub>5</sub>, leading to a larger off-center displacement of the neighboring LiO<sub>6</sub> octahedra and the expansion of unit cell volume. This structural manipulation improves the electrochemical dynamics of Li<sub>3</sub>V<sub>2</sub>O<sub>5</sub> with a better rate capability (143.3 mA h g<sup>-1</sup> for LVON2 vs 94.1 mA h g<sup>-1</sup> for the pristine sample at 1000 mA g<sup>-1</sup>) and a decreased charge-transfer resistance (159.2 Ω for LVON2 vs 278.6 Ω for the pristine sample). Differential scanning calorimetry and finite element analysis also reveal the enhanced thermal stability of Ni-doped Li<sub>3</sub>V<sub>2</sub>O<sub>5</sub> at both material and full battery levels. This advancement lays a solid foundation for the development of Li<sub>3</sub>V<sub>2</sub>O<sub>5</sub>-based cathode materials for high-energy-density lithium-ion batteries.

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Publication Details

Journal
ACS Applied Materials & Interfaces
Published
2025-04-07
DOI
https://doi.org/10.1021/acsami.5c01471
Citations
5
Primary Topic
Advancements in Battery Materials
Type
article
Field-Weighted Citation Impact
3.65

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article

High-Energy-Density Cathode Material Achieved by Upgrading Low-Voltage Li3V2O5 via Ni Doping

Chih‐Fang Huang, Chengzhi Hu, Zeheng Yang, Zhangxian Chen et al.
5 citations
ACS Applied Materials & Interfaces
Advancements in Battery Materials
3.65
article

High-Energy-Density Cathode Material Achieved by Upgrading Low-Voltage Li3V2O5 via Ni Doping

Chih‐Fang Huang, Chengzhi Hu, Zeheng Yang, Zhangxian Chen, Guoxian Wang, Song Chen, Can Wang, Weixin Zhang, Kai‐Xue Wang
article en
5 citations

Abstract

High-energy-density lithium-ion batteries have great need for cathode materials with exceptional specific discharge capacity. Li<sub>3</sub>V<sub>2</sub>O<sub>5</sub> shows great potential because of its high capacity (e.g., 266 mA h g<sup>-1</sup> at 0.1 A g<sup>-1</sup>). However, its low-lying voltage plateau (∼0.6 V vs Li<sup>+</sup>/Li) restricts its use exclusively to anode applications. This work presents for the first time the development of Li<sub>3</sub>V<sub>2</sub>O<sub>5</sub> as a high-energy-density cathode material through Ni doping. Structural analysis reveals that Ni-doped Li<sub>3</sub>V<sub>2</sub>O<sub>5</sub> forms a cation-disordered rock-salt phase with a uniform distribution of Ni. Introducing 1 mol % Ni (denoted as LVON2) prolongs the V-based plateau (∼2.5 V) and results in an additional discharge capacity of 35 mA h g<sup>-1</sup>. In particular, a plateau ascribed to Ni<sup>2+</sup>/Ni<sup>3+</sup> redox reaction emerges at ∼3.5 V, contributing an extra discharge capacity of 42 mA h g<sup>-1</sup>. Consequently, LVON2 achieves high specific discharge capacities of 270.8 mA h g<sup>-1</sup> at 50 mA g<sup>-1</sup> and 339.4 mA h g<sup>-1</sup> at 20 mA g<sup>-1</sup> (corresponding to an energy density of 837 W h kg<sup>-1</sup>), surpassing the pristine Li<sub>3</sub>V<sub>2</sub>O<sub>5</sub> and many latest cathode materials. Density functional theory calculation shows that Ni preferentially occupies the empty tetragonal sites in Li<sub>3</sub>V<sub>2</sub>O<sub>5</sub>, leading to a larger off-center displacement of the neighboring LiO<sub>6</sub> octahedra and the expansion of unit cell volume. This structural manipulation improves the electrochemical dynamics of Li<sub>3</sub>V<sub>2</sub>O<sub>5</sub> with a better rate capability (143.3 mA h g<sup>-1</sup> for LVON2 vs 94.1 mA h g<sup>-1</sup> for the pristine sample at 1000 mA g<sup>-1</sup>) and a decreased charge-transfer resistance (159.2 Ω for LVON2 vs 278.6 Ω for the pristine sample). Differential scanning calorimetry and finite element analysis also reveal the enhanced thermal stability of Ni-doped Li<sub>3</sub>V<sub>2</sub>O<sub>5</sub> at both material and full battery levels. This advancement lays a solid foundation for the development of Li<sub>3</sub>V<sub>2</sub>O<sub>5</sub>-based cathode materials for high-energy-density lithium-ion batteries.

ACS Applied Materials & InterfacesVol. 17(15)
Hefei University of Technology (CN), Catalytic Materials (United States) (US)
National Natural Science Foundation of China, Anhui Provincial Department of Science and Technology, Anhui Provincial Development and Reform Commission, Natural Science Foundation of Anhui Province
Affordable and clean energy
Openalex Percentile: Top 7%
Advancements in Battery Materials
3.65
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