We have studied spectra and angular distribution of emission in
Fabry–Perot cavities formed by two silver mirrors separated by a layer
of poly (methyl methacrylate) polymer doped with rhodamine 6G (R6G)
dye in low (
20
g
/
l
) and high (
200
g
/
l
) concentrations. The frequency of
emission radiated to a cavity mode was larger at large outcoupling
angles—the “rainbow” effect. At the same time, the angle of the
strongest emission was also determined by the cavity size: the larger
the cavity, the larger the angle. The angular distribution of emission
is commonly dominated by two symmetrical lobes (located at the
intersection of the three-dimensional emission cone with a horizontal
plane) pointing to the left and to the right of the normal to the
sample. Despite the strong Stokes shift in R6G dye, the branch of the
cavity dispersion curve obtained in the emission experiment is
positioned above the one obtained in the reflection (extinction)
experiment. Some dye molecules are poorly coupled to cavity modes.
Their emission has very broad angular distribution with the maximum at
θ
=
0
∘
. The signatures of strong
cavity–exciton coupling were observed at high dye concentration (
200
g
/
l
) but not at low concentration (
20
g
/
l
). The evidence of the effect of
strong coupling on emission is exemplified by a strong difference in
the angular distribution of emission in two almost identical cavities,
one with and another without strong coupling. Most importantly, we
have demonstrated the possibility to control the ground state
concentration, the coupling strength, and the dye emission spectra
with Q-switched laser pulses.