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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Two giant atoms in a waveguide-QED system form both static bound states with persistent excitations and oscillating bound states featuring periodic atom-photon exchanges and extra harmonic components from quasi-dark modes.
A scheme for nonreciprocal single-photon routing in an atom-dimer waveguide-QED system achieves complete transmission control via chiral asymmetry without requiring ideal chirality in the non-Markovian regime.
citing papers explorer
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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.
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Oscillating bound states in waveguide-QED system with two giant atoms
Two giant atoms in a waveguide-QED system form both static bound states with persistent excitations and oscillating bound states featuring periodic atom-photon exchanges and extra harmonic components from quasi-dark modes.
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Nonreciprocal routing induced by chirality in an atom-dimer waveguide-QED system
A scheme for nonreciprocal single-photon routing in an atom-dimer waveguide-QED system achieves complete transmission control via chiral asymmetry without requiring ideal chirality in the non-Markovian regime.