Abstract

In this work, we present a combined experimental and theoretical study on the V L2,3-edge x-ray absorption (XAS) and x-ray magnetic circular dichroism (XMCD) spectra of VIVO(acac)2 and VIII(acac)3 prototype complexes. The recorded V L2,3-edge XAS and XMCD spectra are richly featured in both V L3 and L2 spectral regions. In an effort to predict and interpret the nature of the experimentally observed spectral features, a first-principles approach for the simultaneous prediction of XAS and XMCD spectra in the framework of wavefunction based ab initio methods is presented. The theory used here has previously been formulated for predicting optical absorption and MCD spectra. In the present context, it is applied to the prediction of the V L2,3-edge XAS and XMCD spectra of the VIVO(acac)2 and VIII(acac)3 complexes. In this approach, the spin-free Hamiltonian is computed on the basis of the complete active space configuration interaction (CASCI) in conjunction with second order N-electron valence state perturbation theory (NEVPT2) as well as the density functional theory (DFT)/restricted open configuration interaction with singles configuration state functions based on a ground state Kohn-Sham determinant (ROCIS/DFT). Quasi-degenerate perturbation theory is then used to treat the spin-orbit coupling (SOC) operator variationally at the many particle level. The XAS and XMCD transitions are computed between the relativistic many particle states, considering their respective Boltzmann populations. These states are obtained from the diagonalization of the SOC operator along with the spin and orbital Zeeman operators. Upon averaging over all possible magnetic field orientations, the XAS and XMCD spectra of randomly oriented samples are obtained. This approach does not rely on the validity of low-order perturbation theory and provides simultaneous access to the calculation of XMCD A, B, and C terms. The ability of the method to predict the XMCD C-term signs and provide access to the XMCD intensity mechanism is demonstrated on the basis of a generalized state coupling mechanism based on the type of the excitations dominating the relativistically corrected states. In the second step, the performance of CASCI, CASCI/NEVPT2, and ROCIS/DFT is evaluated. The very good agreement between theory and experiment has allowed us to unravel the complicated XMCD C-term mechanism on the basis of the SOC interaction between the various multiplets with spin S' = S, S ± 1. In the last step, it is shown that the commonly used spin and orbital sum rules are inadequate in interpreting the intensity mechanism of the XAS and XMCD spectra of the VIVO(acac)2 and VIII(acac)3 complexes as they breakdown when they are employed to predict their magneto-optical properties. This conclusion is expected to hold more generally.

Highlights

  • The spin-free Hamiltonian is computed on the basis of the complete active space configuration interaction (CASCI) in conjunction with second order N-electron valence state perturbation theory (NEVPT2) as well as the density functional theory (DFT)/restricted open configuration interaction with singles configuration state functions based on a ground state Kohn-Sham determinant (ROCIS/DFT)

  • Owing to the recent technological and methodological developments in the field of x-ray spectroscopy over the last decades, x-ray magnetic circular dichroism (XMCD) has developed into an important experimental analytical tool.[1,2,3,4,5,6] (X)MCD has been used to unravel the electronic structure and magnetic properties of a wide range of materials spanning from molecular complexes to solid-state scitation.org/journal/jcp materials and even to biological metallocofactors.[4,7–33]

  • We have shown that the V L2,3-edge XMCD spectra of the two complexes contain significant information content in both L3- and L2-edge spectral regions, providing well-resolved spectral features with positive and negative C-term XMCD intensities

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Summary

INTRODUCTION

Owing to the recent technological and methodological developments in the field of x-ray spectroscopy over the last decades, x-ray magnetic circular dichroism (XMCD) has developed into an important experimental analytical tool.[1,2,3,4,5,6] (X)MCD has been used to unravel the electronic structure and magnetic properties of a wide range of materials spanning from molecular complexes to solid-state. The theoretical approaches that are currently employed for the calculation of metal L2,3-edge XMCD spectra range between various particle/hole theories and multiplet approaches.[39,56–62] They are based on the same principles used to derive the sum rules and on a perturbative treatment of the SOC splitting within the final state manifold. It is of interest to note that both state average SA-CASSCF/NEVPT2 and MRCI type methods can be used to calculate MCD signs and intensities.[98–101] In this approach, the difference between the LCP and RCP light induced transition probabilities in the presence of a homogeneous external magnetic field are computed using exact diagonalization techniques.[98]. The validity of the sum rules to interpret the magnetic properties of VIVO(acac)[2] and VIII(acac)[3] complexes is critically evaluated

XMCD general expression in the non-relativistic limit
Quasi-degenerate perturbation theory
Calculation of XMCD intensities
RESULTS AND ANALYSIS
Electronic structure
INSIGHTS INTO THE INTENSITY MECHANISM
VALIDITY OF THE XMCD SUM RULES: A CRITICAL EVALUATION
CONCLUSIONS
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