Independent motionless two-level atoms emit thermal light statistics only when atom number and coherent-to-incoherent emission ratio meet specific conditions for each correlation order.
This number is given by Bλ,N = N! [N−ℓ(λ)]! Q n rn! ,(B8) whereℓ(λ)= P n rn is the total number of nonzero ele- ments of the partition
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Deviations from thermal light statistics in ensembles of independent two-level emitters
Independent motionless two-level atoms emit thermal light statistics only when atom number and coherent-to-incoherent emission ratio meet specific conditions for each correlation order.