We consider the resonance fluorescence of a two-level atom in a vacuum with
a high intensity driving field, such that the Rabi frequency of the field
is non-negligible up to frequencies comparable to the transition frequency
of the atom. At these high intensities, the conventional rotating wave appr
oximation cannot be applied to the atom-laser Hamiltonian and the modal den
sities of the vacuum at the dressed transition frequencies differ significa
ntly from each other. On treating the counter-rotating part of the Hamilton
ian as a perturbation and carrying out the Weisskopf-Wigner approximation i
n the dressed states basis, we find that the high driving intensity leads t
o significant deviations from the traditional Mellow resonance fluorescence
spectrum. In particular we find unequally intense Mollow side-bands and th
at the generation of higher order triplets and harmonics is substantially e
nhanced by the high vacuum modal density at the corresponding high resonanc
e frequencies.