Frequency-Dependent Sternheimer Linear-Response Formalism for Strongly Coupled Light-Matter Systems

The rapid progress in quantum-optical experiments, especially in the field of cavity quantum electrodynamics and nanoplasmonics, allows one to substantially modify and control chemical and physical properties of atoms, molecules, and solids by strongly coupling to the quantized field. Alongside such experimental advances has been the recent development of ab initio approaches such as quantum electrodynamical density-functional theory (QEDFT), which is capable of describing these strongly coupled systems from first principles. To investigate response properties of relatively large systems coupled to a wide range of photon modes, ab initio methods that scale well with system size become relevant. In light of this, we extend the linearresponse Sternheimer approach within the framework of QEDFT to efficiently compute excited-state properties of strongly coupled light-matter systems. Using this method, we capture features of strong light-matter coupling both in the dispersion and absorption properties of a molecular system strongly coupled to the modes of a cavity. We exemplify the efficiency of the Sternheimer approach by coupling the matter system to the continuum of an electromagnetic field. We observe changes in the spectral features of the coupled system as Lorentzian line shapes turn into Fano resonances when the molecule interacts strongly with the continuum of modes. This work provides an alternative approach for computing efficiently excited-state properties of large molecular systems interacting with the quantized electromagnetic field.

Automated summary

Recent progress in quantum-optical experiments enables the modification and control of chemical and physical properties of atoms, molecules, and solids by strongly coupling to the quantized field. This study extends the Sternheimer approach to efficiently compute excited-state properties of strongly coupled light-matter systems within the framework of quantum electrodynamical density-functional theory. The method captures the features of strong light-matter coupling and provides an alternative approach for computing excited-state properties of large molecular systems interacting with the quantized electromagnetic field.