In a recent paper Damour and Mukhanov described a scenario where inflation
may continue during the oscillatory phase. This effect is possible because
the scalar field spends a significant fraction of each period of oscillatio
n on the upper part of the potential. Such an additional period of inflatio
n could push perturbations after the slow roll regime to observable scales.
Although in this work we show that the small region of the Damour-Mukhanov
parameter q gives the main contribution to oscillating inflation, it was n
ot satisfactorily understood until now. Furthermore, it gives an expression
for the energy density spectrum of perturbations, which is well behaved in
the whole physical range of q.