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When a resonant continuous wave is input, the normalized second-order correlation function g (2) (τ) of the output is given by g (2) (τ) = (1- e-Γτ) 2 in this system. Therefore, the photon blockade mechanism becomes weaker when d Γ-1.
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When a resonant continuous wave is input, the normalized second-order correlation function g (2) (τ) of the output is given by g (2) (τ) = (1- e-Γτ) 2 in this system. Therefore, the photon blockade mechanism becomes weaker when d Γ-1.
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