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Quantify the sources of large ZFS errors for Sc, Y, and La

Determine and quantify the sources of the large errors observed when predicting the zero-field splitting in the 2D ground term of Sc, Y, and La using the BP2-QDNEVPT2 and DKH2-QDNEVPT2 methods, explicitly assessing the contributions of high-order dynamic correlation effects (such as triple and higher excitations outside the active space) and their interplay with spin–orbit coupling, as suggested by the performance of variational X2C-MRCISD for Sc and La.

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Background

In the transition-metal benchmark (Sc, Y, La; 2D ground term), the authors report that both BP2- and DKH2-QDNEVPT2 significantly deviate from experimental zero-field splittings, and that even variational X2C-MRCISD shows large errors for Sc and La. This points to unresolved methodological issues impacting accuracy.

While the authors hypothesize that high-order dynamic correlation effects beyond doubles (e.g., triples in non-active orbitals) and their interaction with spin–orbit coupling likely contribute, they explicitly state that they cannot quantify the source of these errors. A clear determination and quantification of these effects is needed to guide methodological improvements and benchmarking across these challenging systems.

References

Although we cannot quantify the source of these errors, the poor performance of variational X2C-MRCISD method for Sc and La suggests that they are at least in part due to high-order dynamic correlation effects, such as triple (and higher) excitations in non-active orbitals, and their interplay with spin--orbit coupling.

Consistent Second-Order Treatment of Spin-Orbit Coupling and Dynamic Correlation in Quasidegenerate N-Electron Valence Perturbation Theory (2404.04716 - Majumder et al., 6 Apr 2024) in Section 4.2 (Transition Metal Elements)