The advantages of the weakly coupled two resonant optical cavities (hereina
fter referred to as three-mirror cavity) used for observation of the supern
arrow saturated absorption resonances are shown. Among these advantages we
can name: (a) the possibility to control the intensity in the cavity with t
he inside absorbing cell which is important when the gain and absorption sa
turation parameters differ significantly; (b) the resonances observation fr
om the 'passive' side of the three-mirror cavity permits us to decrease dra
stically the influence of the reflected signal from the detector; (c) if in
stead of the absorbing cell an active system is put in (gain plus absorptio
n), it is possible by tuning the operating mode of the active interferomete
r to obtain many-fold gain of the supernarrow resonance amplitude.