Using electron-filling modulation absorption spectroscopy, we study the eff
ect of quantum dot charging on the interband excitonic transitions in type-
II Ge/Si heterostructures containing pyramidal Ge nanocrystals. In contrast
to type-I systems, the ground-state absorption is found to be blueshifted
when exciton-hole and exciton-exciton complexes are formed. For a positivel
y charged dot, we argue that this is the consequence of the dominance of th
e hole-hole interaction compared to the electron-hole interaction due to th
e spatial separation of the electron and hole. The large oscillator strengt
h (0.5) and the exciton binding energy (25 meV) are determined from the exp
erimental data. The results are explained by effects of the electron and ho
le localization and by electron wave-function leakage in the dots. The elec
tronic structure of spatially indirect excitons is calculated self-consiste
ntly in the effective-mass approximation for pyramidal-shaped Ge/Si quantum
dots. The inhomogeneous strain distribution in the quantum dot layer has b
een taken into account through modification of the confining potential. The
calculations show that the electron of an indirect exciton resides in the
Si near to the Ge pyramid apex due to maximum strain in this region, while
the hole is confined close to the pyramid base. The electron-hole overlap i
s calculated to be 15%. When two excitons are excited in the dot, the elect
rons are found to be spatially separated and have different single-particle
quantization energies. We argue that this is the reason why the biexciton
absorption is blueshifted as compared to a single exciton. A satisfying agr
eement is found between theoretical and experimental data.