We revisit the problem of spontaneous emission by a two-level system i
n a cavity, concentrating in particular on those aspects associated wi
th the finite propagation time of light between the atom and the cavit
y boundaries. We find that spontaneous emission always occurs first at
the free space rate and there is then an abrupt change in these dynam
ics when light reflected by the cavity mirrors returns to the atom, le
ading to interference effects that result either in an enhancement or
a reduction of this rate or in a periodic exchange of excitation betwe
en the atom and the cavity field. From this point of view, reversible
spontaneous emission in terms of single-mode ''vacuum Rabi oscillation
s'' can be interpreted as resulting from the interference between the
multimode partial waves reflected at the cavity mirrors and the instan
taneously radiated light.