Employing the path integral approach, we calculate the semiclassical e
quilibrium density matrix of a particle moving in a nonlinear potentia
l field for coordinates near the top of a potential barrier As the tem
perature is decreased, near a critical temperature T-c the harmonic ap
proximation for the fluctuation path integral fails. This is due to a
caustic arising at a bifurcation point of the classical paths. We prov
ide a selfconsistent scheme to treat the large quantum fluctuations le
ading to a nonlinear fluctuation potential. The procedure differs from
methods used near caustics of the real time propagator. The semiclass
ical density matrix is determined explicitly for the case of asymmetri
c barriers from high temperatures down to temperatures somewhat below
T-c.