Abstract

A detailed study of the electronic and geometric structure of V2O5 and its X-ray spectroscopic properties is presented. Cluster models of increasing size were constructed in order to represent the surface and the bulk environment of V2O5. The models were terminated with hydrogen atoms at the edges or embedded in a Madelung field. The structure and interlayer binding energies were studied with dispersion-corrected local, hybrid and double hybrid density functional theory as well as the local pair natural orbital coupled cluster method (LPNO-CCSD). Convergence of the results with respect to cluster size was achieved by extending the model to up to 20 vanadium centers. The O K-edge and the V L2,3-edge NEXAFS spectra of V2O5 were calculated on the basis of the newly developed Restricted Open shell Configuration Interaction with Singles (DFT-ROCIS) method. In this study the applicability of the method is extended to the field of solid-state catalysis. For the first time excellent agreement between theoretically predicted and experimentally measured vanadium L-edge NEXAFS spectra of V2O5 was achieved. At the same time the agreement between experimental and theoretical oxygen K-edge spectra is also excellent. Importantly, the intensity distribution between the oxygen K-edge and vanadium L-edge spectra is correctly reproduced, thus indicating that the covalency of the metal-ligand bonds is correctly described by the calculations. The origin of the spectral features is discussed in terms of the electronic structure using both quasi-atomic jj coupling and molecular LS coupling schemes. The effects of the bulk environment driven by weak interlayer interactions were also studied, demonstrating that large clusters are important in order to correctly calculate core level absorption spectra in solids.

Highlights

  • density functional theory (DFT)/ROCIS calculations were performed using the converged restricted Kohn–Sham RKS wavefunctions using the B3LYP/ def2-TZVP calculation protocol together with the auxiliary basis set def2-TZVP/J in order to accelerate the calculations in the framework of RI approximation

  • point charge field (PC) are chosen over the corresponding atom position on extended crystal super cells; the choice of the magnitude of these charges in either the boundary region (BR) or PCs has been intensively debated in the literature.[86]

  • These results demonstrate the suitability of the V4O18H16 cluster model to describe the X-ray bulk structure of V2O5

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Summary

First principles calculations of the structure and

Cite this: Phys.Chem.Chem.Phys.,2013, V L-edge X-ray absorption spectra of V2O5 using local. A detailed study of the electronic and geometric structure of V2O5 and its X-ray spectroscopic properties is presented. Cluster models of increasing size were constructed in order to represent the surface and the bulk environment of V2O5. Convergence of the results with respect to cluster size was achieved by extending the model to up to 20 vanadium centers. In this study the applicability of the method is extended to the field of solid-state catalysis. For the first time excellent agreement between theoretically predicted and experimentally measured vanadium L-edge NEXAFS spectra of V2O5 was achieved. At the same time the agreement between experimental and theoretical oxygen K-edge spectra is excellent. The effects of the bulk environment driven by weak interlayer interactions were studied, demonstrating that large clusters are important in order to correctly calculate core level absorption spectra in solids

Introduction
Jpttq À cHFKpttq t
Computational details
Geometric properties
Construction of cluster models
Weak interlayer interactions
Electronic structure
Hydrogen saturated clusters
Cluster models
Bulk environment
Embedded clusters
Point charges effect
Lowdin bond orders
Conclusion on the choice of cluster modeling Abbreviations
Findings
Conclusions

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