The intended quantity is , the threshold population inversion density of the cavity after switching to low loss. At this value stimulated gain exactly balances the photon-loss rate:Above threshold a nonzero seed grows; below threshold it decays. The unstarred in the subpart is shorthand for the starred threshold quantity in the displayed equations, rather than a different total atomic population. The photon lifetime fixes the photon-density loss rate .
Write , and during this derivation. Eliminating the stimulated term between the two laser rate equations gives the photon balanceIntegrate over the pulse, taking negligible initial and final stored photon densities:The photons lost from the cavity carry total energy . Since ,This identifies the supplied energy formula under the ideal extraction convention that all photon loss is useful output. If only a fraction of the loss exits the output coupler, the measured output energy is . The rate equations by themselves do not distinguish useful output from parasitic loss.
The Q-switched energy extraction efficiency in the ideal loss convention of ii isThe first factor reflects the definition of inversion: one stimulated transition reduces the upper population and increases the lower population, changing by . Thus one emitted photon consumes units of inversion. The second factor accounts for the inversion left after the pulse; finite pumping above threshold does not generally extract all the initially stored inversion. This is not the wall-plug efficiency and does not include the energy cost of pumping or the factor for imperfect output extraction.
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