Abstract
The eigenvalue equation for absorptive bistability in a ring cavity is analyzed in the mean-field limit. Perturbative solutions are obtained in two distinct limits: κγ,γ and κγ,γ, where κ and γ,γ are field and atomic damping rates, respectively. For κγ,γ, the eigenvalues satisfy a cubic equation, derived previously in the theory of self-pulsing in absorptive bistability. For κγ,γ, while the "dressed-field-mode" eigenvalues are solutions to this cubic equation, the "dressed-atomic-mode" eigenvalues are not.

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