The purpose of this work is to clarify the type of corresponding radiative transitions and the PL mechanism in the big silicon nano-crystallites with the size from the range of 10-150 nm, which is higher than an exciton Bohr radius (≤ 5 nm) in corresponding bulk crystal. Photoluminescence in this type of Si nanocrystals is analyzed from the point of view of new concept based on the hot carrier ballistic transport role in the excitation of oxide-related defects at the Si/SiOx interface. The role of hot carrier ballistic transport in the modification of photocurrent spectra of Si NC device structures is discussed as well. . Optical properties of such systems are sensitive to NC size fluctuations, defects and surface effects due to large surface to volume ratio in small NCs. The first experiments connected with joint investigation of optical absorption and photoluminescence (PL) spectra of porous Si (PSi) films with different crystallite sizes (2.0, 3.5 and 9.0 nm) have shown a gradual increase in the absorption coefficient near the absorption edge and in higher energy range with the decrease in the average diameter of Si NCs [4]. At the same time no significant size dependence of the PL peak energy was observed. In thermal oxidation experiments and at native oxidation (aging) the size of Si NCs decreases and this process has to accompany by the blue shift of PL bands in the case of quantum confinement PL model. The luminescence behaviour of oxidized PSi has been examined, but in many cases no blue shifting of the PL has been noted [5,6]. Thus some questions about correlation of peak position of PL band caused by exciton recombination inside of Si NCs with their sizes, the nature of other PL bands as well as relative contribution of different elementary PL bands into total PL spectrum are still not clear. As a rule two groups of Si NC systems have to be discussed. The first class of systems deals with Si NCs of the small size (a ≤ a B , where a B is the exciton Bohr radius equal to 4.8 nm for the bulk Si). The optical properties in such NCs are controlled by the quantum confinement effect. The second class of systems deals with NCs of the big size (a > a B ) from the range of 10-150 nm. For this case the quantum confinement model in emission and electronic transport do not work and carrier ballistic effect dominates [5][6][7].The paper presents the comparison of results for integrated PL intensity dependences versus Si NC sizes (30-350 nm) for the 1.7 eV PL band in PSi obtained experimentally and numerically calculated on the base of hot carrier ballistic PL model [5,6].