where the effective forward rate constant decreases as the inverse square of Γ as Γ increases. In addition, a similar dependence on Q is expected for different V l where the transition point along Q is located around Q ∼ hω c /V l . Overall, Fig. demonstrates that the suppression effect of cavity loss as seen in Fig. and Fig. can be alleviated, either partially or entirely, by replenishing the UP population with a CW laser tuned to the UP frequency.