A theoretical study of the coherent light scattering from disordered photon
ic crystals is presented. In addition to;the conventional enhancement of th
e reflected light intensity into the backscattering direction, the so-calle
d coherent backscattering (CBS), the periodic modulation of the dielectric
function in photonic crystals gives rise to a qualitatively new effect: enh
ancement of the reflected light intensity in directions different from the
backscattering direction. These additional coherent scattering processes, d
ubbed here umklapp scattering (CUS), result in peaks, which are most pronou
nced when the incident light beam enters the sample at an angle close to th
e the Bragg angle. Assuming that the dielectric function modulation is weak
, we study the shape of the CUS peaks for different relative lengths of the
modulation-induced Bragg attenuation compared to the disorder-induced mean
free path. We show that when the Bragg length increases, then the CBS peak
assumes its conventional shape, whereas the CUS peak rapidly diminishes in
amplitude. We also study the suppression of the CUS peak upon the departur
e of the incident beam from the Bragg resonance: we found that the diminish
ing of the CUS intensity is accompanied by substantial broadening. In addit
ion, the peak becomes asymmetric.