This work demonstrates the effectiveness of a new g-ROHF response theory for electric and magnetic properties, highlighting its advantage for complex open-shell systems.
In this work, the formal development and implementation of a general restricted open-shell Hartree–Fock (g-ROHF) response theory is presented. The theory enables analytic computation of electric and magnetic response properties for arbitrarily complex open-shell configurations. In contrast to traditional ROHF methods, which are typically restricted to high-spin cases, the g-ROHF formulation supports general-spin couplings and orbital degeneracies while preserving the spin purity. A new set of vector-coupling coefficients is introduced that allows for the calculation of a proper spin density from a g-ROHF wave function. Analytic nuclear derivatives, along with the electric and magnetic orbital Hessians, are derived in a unified framework. Special attention is given to the treatment of SCF instabilities and the projection of unphysical modes from the response space. An efficient AO-driven implementation is described and validated across a broad range of open-shell systems, including small molecules, transition-metal complexes, and metal–radical assemblies. Specifically, the method is applied to the calculation of g-tensors and hyperfine couplings (including spin–orbit coupling corrections) in experimentally well-characterized systems such as mixed-valence manganese(III/IV) dimers and the metal–radical complex Fe(GMA)(pyridine)+. The g-ROHF framework provides a robust, efficient, and physically rigorous platform for treating the electronic structure and properties of complex open-shell molecules and serves as a convenient foundation for the development of post-Hartree–Fock correlation methods. The present work sets the stage for extensions to excited-state response theory, DFT-based treatments, and coupled-cluster response formulations.
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Frank Neese (2025) studied this question.
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