We develop a quantum theory of a single-mode thresholdless laser. We start
from basic Heisenberg-Langevin equations of motion for the field and atomic
operators, and obtain an approximate analytical solution to these operator
equations. We compare the predictions of this model for the intensity and
power spectrum of the field to the results of a Monte Carlo numerical simul
ation of the original Heisenberg-Langevin equations, and find them in excel
lent agreement. We also compare these predictions to those of a rate-equati
on model, which takes into account spontaneous emission. We show that our m
odel gives more reliable results in the bad cavity limit at high intensitie
s. Based upon these results, we propose a simple characterization of the th
resholdless behavior. Finally, we apply our model to microsphere Nd-doped l
asers at low temperatures, which are promising devices for a well-controlle
d thresholdless operation. [S1050-2947(99)10502-X].