In the computational chemistry of molecular materials, strong static correlation effects appear when electronic states, often involving the ground state, become quasidegenerate, as occurs, for example, in bond-breaking processes. Such situations present significant challenges for accurate theoretical treatment. In these regimes, many-body methods involving a single-determinant description, such as Hartree-Fock theory and its time-dependent extension, fail to reproduce the correct topology of the ground and excited state potential energy surfaces (e.g., near conical intersections). When strongly correlated electronic systems are further strongly coupled to a quantized radiation field within the framework of nonrelativistic cavity quantum electrodynamics, an additional photonic degree of freedom introduces both new complexity and new opportunities for control. Excited cavity photons can modify bond-breaking processes and enable tunability of geometrical and spin-phase transitions, for instance, in organometallic complexes. To overcome this bottleneck, in this work, we extend the well-studied spin-flip configuration interaction singles (SF-CIS) approach to explicitly include quantized cavity photons leading to the QED-SF-CIS method. We derive the spin-flip Hamiltonian and find that the double excitation subspace of the hybrid system (i.e., mixed electron-photon single-single excitations) must be included in the configurations to properly describe singlet electronic states interacting with cavity photons. We then illustrate, through representative molecular examples, how cavity coupling can provide additional tunability in bond-breaking processes. We finally generalize this approach to include higher numbers of photonic excitations, which are required in the strong coupling regime and at higher-excitation frequencies.

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• Electronic structure of atoms & molecules
• Light-matter interaction