The uncharted space of non-Hermitian solutions to the Hartree–Fock and Kohn–Sham equations
Many problems in physical chemistry involve systems that are coupled to an environment, such as a molecule interacting with an adjacent surface, possibly resulting in meta-stable molecular states where electron density is transferred to the surface. Such systems can be described by non-Hermitian quantum mechanics (NHQM), where the Hamiltonian includes a complex potential. Within NHQM, one can also formulate the Hartree-Fock (HF) and Kohn-Sham (KS) methods and, as in the conventional theory, an effective independent-particle picture is employed. The crucial observation of the present study is that even for systems that are not coupled to an environment, in the non-Hermitian HF or KS equation, a single electron is interacting with the remaining electrons, which act as an environment, allowing for the exchange of current density between the one-electron and the remaining (N - 1)-electron system. The corresponding self-consistent states represent a new uncharted space of solutions to the HF and KS equations. We show that the additional solutions can have a physical interpretation and, therefore, extend the range of problems HF and KS can be applied to. If open-system HF and KS calculations are performed, the new class of solutions is always encountered, but this has also not been noted previously.
Authors
- Pierre-Olivier Roy (ORCID: https://orcid.org/0009-0007-2055-6611)
- Didier Mayou (ORCID: https://orcid.org/0000-0003-2723-9727)
- Matthias Ernzerhof (ORCID: https://orcid.org/0000-0001-5679-8902)
- Mohamed Loutis (ORCID: https://orcid.org/0009-0001-6491-9193)
Institutions
- University of Geneva (CH)
- Université du Québec à Montréal (CA)
- Institut Néel (FR)
- Université de Montréal (CA)
Publication Details
- Journal
- The Journal of Chemical Physics
- Published
- 2025-12-01
- DOI
- https://doi.org/10.1063/5.0272598
- Primary Topic
- Quantum Mechanics and Non-Hermitian Physics
- Type
- article
- Field-Weighted Citation Impact
- 0.00