Se. Hodges et al., TURN-ON TRANSIENT DYNAMICS IN A MULTIMODE, COMPOUND-CAVITY LASER, Journal of the Optical Society of America. B, Optical physics, 14(1), 1997, pp. 180-190
The turn-on-time statistics for an individual longitudinal mode and th
e total intensity of a multimode laser are shown to be very different.
In both experiment and theory we find that the differences are due ma
inly to transitory modes that decay as a result of frequency-dependent
losses and gains. Associated with this phenomenon is a kink in the ti
me evolution of the mode intensity, but net in the total intensity, th
at represents a transition in the dynamics from domination by independ
ent growth of all modes to domination by competition between modes wit
h different net gains. This unequal competition increases the average
and the standard deviation of the individual mode turn-on time. The ex
perimental dye-laser system has a thin gain medium (100 mu m) that is
strongly coupled to a short cavity (2.5 cm) and is adjacent to one of
the cavity mirrors. The opposite cavity mirror serves as a relatively
weak output coupler. The presence of the thin gain medium in the cavit
y causes the effective pump and loss rates to be frequency dependent.
The result is a transient spectrum in which the cavity modes that have
the highest net gain dominate the system more as the turn-on transien
t progresses. The gain spectrum is found to be strongly affected by th
e frequency dependence of the compound-cavity modes. Using realistic l
aser parameters, numerical simulations of a multimode laser model {dev
eloped in companion paper [J. Opt. Soc. Am. B 14, 191 (1997)]} yield t
urn-on dynamics and statistics that agree well with those measured exp
erimentally. (C) 1997 Optical Society of America.