Consider a density-dependent birth-death process
XN on a finite state
space of size
N. Let
PN be the law (on
D([0,
T]) where
T>0 is
arbitrary) of the density process
XN/
N and let

be the unique
stationary distribution (on [0,1]) of
XN/
N, if it exists. Typically,
these distributions converge weakly to a degenerate distribution as

,
so the probability of sets not containing the
degenerate point will tend to 0; large deviations is concerned with
obtaining the exponential decay rate of these probabilities. Friedlin-Wentzel
theory is used to establish the large deviations behaviour (as

)
of
PN. In the one-dimensional case, a large deviations principle
for the stationary distribution

is obtained by elementary explicit
computations. However, when the birth-death process has an absorbing
state at 0 (so

no longer exists), the same elementary computations
are still applicable to the quasi-stationary distribution, and we show
that the quasi-stationary distributions obey the same large deviations
principle as in the recurrent case. In addition, we address some questions
related to the estimated time to absorption and obtain a large deviations
principle for the invariant distribution in higher dimensions by studying
a quasi-potential.