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Light-matter correlations in Quantum Floquet engineering of cavity quantum materials
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Quantum Floquet engineering (QFE) seeks to generalize the control of quantum systems with classical external fields, widely known as Semi-Classical Floquet engineering (SCFE), to quantum fields. However, to faithfully capture the physics at arbitrary coupling, a gauge-invariant description of light-matter interaction in cavity-QED materials is required, which makes the Hamiltonian highly non-linear in photonic operators. We provide a non-perturbative truncation scheme of the Hamiltonian, which is valid or arbitrary coupling strength, and use it to investigate the role of light-matter correlations, which are absent in SCFE. We find that even in the high-frequency regime, light-matter correlations can be crucial, in particular for the topological properties of a system. As an example, we show that for a SSH chain coupled to a cavity, light-matter correlations break the original chiral symmetry of the chain, strongly affecting the robustness of its edge states. In addition, we show how light-matter correlations are imprinted in the photonic spectral function and discuss their relation with the topology of the bands.
Forward citations
Cited by 3 Pith papers
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Composite-Fermion Study of Cavity-Modified Fractional Quantum Hall Excitation Gaps
Cavity-mediated attractive interactions enhance the fractional quantum Hall transport gap with a quadratic electron-number scaling and a fourth-power dependence on the vacuum-field gradient, as shown by composite-ferm...
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Floquet Theory of lattice electrons coupled to an off-resonant cavity
An off-resonant cavity mediates electron-electron interactions at first order in 1/omega_c, and for an SSH chain these interactions reshape the topological phase diagram at strong coupling.
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A Theoretical Study of Cavity-modulated Topological Anderson Insulators
Cavity photons renormalize hopping amplitudes in a disordered long-range SSH chain and thereby shift topological phase boundaries and the critical disorder for topological Anderson insulator transitions.
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