In this study, we present the superradiance effects of N identical molecular emitters inside Fabry–Pérot
(FP) cavity systems in the framework of macroscopic quantum electrodynamics.
The proposed theory can estimate the enhancement of spontaneous emission
rates, including the effects of cavity geometry and material dielectric
properties. Moreover, our study connects the multichromophoric excitation
energy transfer theory and the Tavis–Cummings model via identical
cooperative decay rates and dipole–dipole shifts. For molecules
resonant with the cavity photon mode, we find that the enhancement
is not exactly proportional to N even in a perfect
FP cavity due to the effects of electrostatic dipole–dipole
interactions. Moreover, in a silver FP cavity, our simulation shows
that the enhancement saturates for a large N, indicating
that the cavity photon mode can lead to only the collective emission
of a limited number of molecules. For molecules in the proximity of
the silver mirror, we demonstrate that under specific conditions,
the subradiance of molecular emitters can occur through surface plasmon
polaritons. Our study not only provides new insights into the mechanism
of superradiance effects but also demonstrates that collective effects
such as superradiance and subradiance can be controlled by manipulating
the dielectric environments.