We discuss the frequency dependence of the spontaneous-emission rate (power
) in a Fabry-Perot microcavity containing a Lorentz dielectric, with emphas
is on modifications of the spectrum under the circumstances of the strong m
edium-cavity coupling. With the standard-cavity tuning, the total spontaneo
us-emission power spectrum consists of a multiwave version of the familiar
low-frequency vacuum Rabi split peak and a broad structure on the high-freq
uency side coming from the enhanced spontaneous emission into the continuum
of the obliquely propagating waves. This form of the spectrum derives from
the properties of the (single-wave) radiation-intensity spectrum of the mo
lecule. Depending on the observation direction, the radiation-intensity spe
ctrum exhibits either a double-peak structure characteristic of the vacuum
Rabi splitting, as observed in light transmission and reflection experiment
s, or a single-peak structure describing the enhanced spontaneous emission
at the corresponding cavity resonant frequency. [S1050-2947(99)02809-7].