Jointly tuning geometric and optical asymmetries in silicon nanoantennas enables Q factors up to 76,000 at wavelength-scale volumes and 10^6 at subwavelength volumes in free-space resonators.
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Quasi-BICs realized in GHz Lamb-wave PnCs on suspended LiNbO3 by decoupling symmetric and antisymmetric modes and controlled symmetry breaking, enabling traveling-wave excitation and frequency-multiplexed resonators.
Coupling phase in a two-giant-atom waveguide-QED system controls the number and profiles of bound states in the continuum and produces a range of quantum dynamical behaviors.
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$Q$ Factors Exceeding $10^{4}$ in Wavelength-to-Subwavelength-Scale Free-Space Resonators
Jointly tuning geometric and optical asymmetries in silicon nanoantennas enables Q factors up to 76,000 at wavelength-scale volumes and 10^6 at subwavelength volumes in free-space resonators.
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Deployable Nanoelectromechanical Bound States in the Continuum Enabled by GHz Lamb Wave Phononic Crystals on LiNbO3 Thin Films
Quasi-BICs realized in GHz Lamb-wave PnCs on suspended LiNbO3 by decoupling symmetric and antisymmetric modes and controlled symmetry breaking, enabling traveling-wave excitation and frequency-multiplexed resonators.
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Bound state in the continuum and dynamics via phase modulation in giant-atom waveguide setups
Coupling phase in a two-giant-atom waveguide-QED system controls the number and profiles of bound states in the continuum and produces a range of quantum dynamical behaviors.