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This research proposes using ultracold atoms in optical lattices to engineer high-order Van Hove singularities, thereby enhancing cavity-polariton hybridization while suppressing absorption losses common in solid-state systems. By controlling band dispersion at the gap edge, the study establishes a new pathway for manipulating polaritons with applications specifically targeted toward quantum nonlinear optics. The work represents a significant theoretical advancement in leveraging quantum gas platforms to optimize light-matter interaction regimes without relying on traditional semiconductor materials.
Formation of Cavity-Polaritons via High-Order Van Hove Singularities
arXiv:2509.15849v3 Announce Type: replace-cross Abstract: We consider polaritons formed by hybridizing a continuum of interband particle-hole excitations of an insulating phase with a cavity photon at subgap frequencies, where absorption is suppressed. The strength of the hybridization is driven by the Van Hove singularity in the joint density of states (JDOS) at the band gap: the stronger the singularity, the more a photon is hybridized with the interband transitions. In order to increase the singularity and thus the polariton hybridization without absorption, we propose to engineer a nonparabolic momentum dispersion of the bands around the gap in order to implement a high-order Van Hove singularity (HOVHS) in the JDOS. Ultracold atoms in tunable optical lattices are an ideal platform to engineer two-dimensional gapped phases with nontrivial band dispersions at the gap. Moreover, the intrinsic noninteracting nature of polarized fermionic atoms prevents the emergence of subgap excitations, which are common in solid-state systems and could otherwise spoil the absence of absorption below the gap. Our findings identify band-engineering at the gap edge as a promising route for polariton control with applications in quantum nonlinear optics.
Abstract:We consider polaritons formed by hybridizing a continuum of interband particle-hole excitations of an insulating phase with a cavity photon at subgap frequencies, where absorption is suppressed. The strength of the hybridization is driven by the Van Hove singularity in the joint density of states (JDOS) at the band gap: the stronger the singularity, the more a photon is hybridized with the interband transitions. In order to increase the singularity and thus the polariton hybridization without absorption, we propose to engineer a nonparabolic momentum dispersion of the bands around the gap in order to implement a high-order Van Hove singularity (HOVHS) in the JDOS. Ultracold atoms in tunable optical lattices are an ideal platform to engineer two-dimensional gapped phases with nontrivial band dispersions at the gap. Moreover, the intrinsic noninteracting nature of polarized fermionic atoms prevents the emergence of subgap excitations, which are common in solid-state systems and could otherwise spoil the absence of absorption below the gap. Our findings identify band-engineering at the gap edge as a promising route for polariton control with applications in quantum nonlinear optics.
Quantum Gases (cond-mat.quant-gas); Optics (physics.optics); Quantum Physics (quant-ph)
arXiv:2509.15849 [cond-mat.quant-gas]
(or arXiv:2509.15849v3 [cond-mat.quant-gas] for this version)
https://doi.org/10.48550/arXiv.2509.15849 Focus to learn more arXiv-issued DOI via DataCite
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