ABSTRACT
When an emitter is coupled to a low Q cavity, cavity damping
dominates the dynamics and the system is in the weak coupling
regime. As discussed in Section 4.4.5, in the weak coupling regime
the spontaneous emission into the cavity mode is enhanced by the
Purcell factor Eq. 4.120. To achieve Purcell factors F 1, either the mode volume must be small or the quality factor must be high.
These conditions are ideally fulfilled by the micro-and nanocavities
introduced in the previous part.