The properties of a passive cesium ARF (atomic resonance filter) are d
etermined predominantly by the physical processes of absorption, emiss
ion and internal energy conversion in the cesium vapor. A fast efficie
nt passive cesium ARF at 455 nm and 459 nm is demonstrated by the meth
od of mixing molecular gas in the cesium vapor. The nominal maximum in
formation rate of the passive cesium ARF, which is an important parame
ter for laser communication applications, is estimated by the fwhm (fu
ll width at half maximum) of the time-resolved fluorescence spectrum o
f its output emission at 852 nm.