Dark states are derived for two-to-four atom cases and the single-excitation subspace of general N-atom cavity-Rydberg systems, with a characterization method via state populations.
We point out that these two states|L (1) [2](1)⟩and|L (1) [2](2)⟩are the Bell states [86], which are maximally entangled states involving two atoms
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Harnessing dark states: coherent control in coupled cavity-Rydberg-atom systems
Dark states are derived for two-to-four atom cases and the single-excitation subspace of general N-atom cavity-Rydberg systems, with a characterization method via state populations.