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XPS Binding Energy Shifts in 2D Ti<sub>3</sub>C<sub>2</sub>T<sub>z</sub> MXene go largely Beyond Intuitive Explanations: Rationalization from DFT Simulations and Experiments

Florian BretteNantes Université CNRS Institut des Matériaux de Nantes Jean Rouxel IMN Nantes F‐44000 FranceStéphane CelerierInstitut de Chimie des Milieux et Matériaux de Poitiers (IC2MP) Université de Poitiers CNRS Poitiers F‐86073 FranceChristine CanaffInstitut de Chimie des Milieux et Matériaux de Poitiers (IC2MP) Université de Poitiers CNRS Poitiers F‐86073 FranceLola LoupiasInstitut de Chimie des Milieux et Matériaux de Poitiers (IC2MP) Université de Poitiers CNRS Poitiers F‐86073 FranceMichaël ParisNantes Université CNRS Institut des Matériaux de Nantes Jean Rouxel IMN Nantes F‐44000 FranceAurélien HabriouxInstitut de Chimie des Milieux et Matériaux de Poitiers (IC2MP) Université de Poitiers CNRS Poitiers F‐86073 FranceFlorent BoucherNantes Université CNRS Institut des Matériaux de Nantes Jean Rouxel IMN Nantes F‐44000 FranceVincent MauchampUniversité de Poitiers ISAE‐ENSMA CNRS PPRIME Poitiers F‐86073 France
2024en
ABI

Аннотация

Abstract MXenes are prototypes of surface tunable 2D materials with vast potential for properties tuning. Accurately characterizing their surface functionalization and its role in electronic structure is crucial, X‐ray photoelectron spectroscopy (XPS) being among the go‐to methods to do so. Despite extensive use, XPS analysis remains however intricate. Focusing on the benchmark MXene Ti 3 C 2 T z , Density Functional Theory (DFT) calculations of core‐level binding energy shifts ( BE .s.) are combined with experiments in order to provide a quantitative interpretation of XPS spectra. This approach demonstrates that BE .s. are driven by the complex interplay between chemical, structural, and subtle electronic structure effects preventing analysis from intuitive arguments or comparison with reference materials. In particular, it is shown that O terminations induce the largest BE .s. at Ti 2p levels despite lower electronegativity than F. Additionally, F 1s levels show weak sensitivity to the F local environment, explaining the single contribution in the spectrum, whereas O 1s states are significantly affected by the local surface chemistry. Finally, clear indicators of surface group vacancies are given at Ti 2p and O 1s levels. These results demonstrate the combination of calculations with experiments as a method of the highest value for MXenes XPS spectra analysis, providing guidelines for otherwise complex interpretations.

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