We present an analysis of strong nonlinear optical effects observed in
the photoluminescence of porous Si. Two groups of effects are discuss
ed. The first includes photoluminescence saturation, suppression of th
e polarization memory, and pump coincident optically induced polarizat
ion anisotropy all observed at room temperature. These effects are wel
l described by nonradiative Auger quenching of the photoluminescence i
n nanocrystals containing more than one electron-hole pair and which a
re selectively excited by linearly polarized light. The second group i
s connected with photoluminescence degradation and a persistent optica
lly induced polarization anisotropy at helium temperature. These effec
ts arise from and are very well described by Auger autoionization of c
rystals selectively excited by polarized light, and subsequent Auger q
uenching of all radiative recombination in them since they contain lon
g-lived charged carriers. Upon heating the samples to room temperature
the electron returns back to the nanocrystal. This restores the initi
al photoluminescence intensity and washes out the long-lived optically
induced polarization anisotropy. The high efficiency of all these eff
ects is provided by the large ratio of the rate of Auger processes to
the radiative recombination rate in the nanosize Si crystals.