2024
DOI: 10.1016/j.jallcom.2024.173697
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Unraveling the potential of Al2CO bilayer as anode material in magnesium ion battery and unsuitability for lithium ion battery

Abdul Majid,
Muhammad Ramzan,
Sheraz Ahmad
et al.
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Cited by 9 publications
(1 citation statement)
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“…As the GGA method was expected to underestimate the band gap of insulators, the Hubbard model was adopted to account for the Coulombic or repulsive interactions of the on-site d electrons. DFT + U has been proposed to improve the description of systems with strongly correlated d electrons. However, due to the lack of a reasonable U value between calculations and experiments, the U parameter was determined through linear response approach for the Rh atom in NaRhO 2 . Evaluation of the U parameter can be performed relying on the definition of U as the difference of the double derivatives of the total energy over the density of the interacting and noninteracting multielectron system, U = 2 E int q normalI 2 2 E non q normalI 2 where q I is the variation in electron density localized on atom I. Equivalently, U can be expressed as the difference in the second derivatives of the localized electron energies with respect to the density of the noninteracting and interacting systems U = 2 α normalI non q normalI 2 2 α normalI int q normalI 2 A linear response approach provides such an alternative route. , The U parameter can be evaluated as the difference in the diagonal elements of the inverse response functions for the noninteracting and interacting systems U = false( χ 1 non χ 1 int false) II …”
Section: Computational Detailsmentioning
confidence: 99%
“…As the GGA method was expected to underestimate the band gap of insulators, the Hubbard model was adopted to account for the Coulombic or repulsive interactions of the on-site d electrons. DFT + U has been proposed to improve the description of systems with strongly correlated d electrons. However, due to the lack of a reasonable U value between calculations and experiments, the U parameter was determined through linear response approach for the Rh atom in NaRhO 2 . Evaluation of the U parameter can be performed relying on the definition of U as the difference of the double derivatives of the total energy over the density of the interacting and noninteracting multielectron system, U = 2 E int q normalI 2 2 E non q normalI 2 where q I is the variation in electron density localized on atom I. Equivalently, U can be expressed as the difference in the second derivatives of the localized electron energies with respect to the density of the noninteracting and interacting systems U = 2 α normalI non q normalI 2 2 α normalI int q normalI 2 A linear response approach provides such an alternative route. , The U parameter can be evaluated as the difference in the diagonal elements of the inverse response functions for the noninteracting and interacting systems U = false( χ 1 non χ 1 int false) II …”
Section: Computational Detailsmentioning
confidence: 99%