We describe the role of first non-Markovian corrections to resonance fluore
scence in photonic crystals, using a perturbative expansion of the Heisenbe
rg equations of motion in powers of die atom-field reservoir coupling,,stre
ngth. Non-Markovian effects arise from the rapid variation of the photonic
density of states with frequency. Our method recaptures the physics of the
photon-atom bound state in the presence of a full photonic band cap, For th
e anisotropic three-dimensional photonic band gap, it predicts remarkable f
eatures in the resonance fluorescence, such as atomic population inversion
and switching behavior in a two-level atom for moderate values of the appli
ed laser field. The magnitude of the switching effect depends sensitively o
n the external laser intensity and its detuning frequency from the atomic t
ransition. The robustness of this effect against nonradiative decay and dep
hasing mechanisms is also investigated.