“…It is observed that the ZnO:Eu 3+ samples doped with 1, 3, 5, 7 and 10 wt% are all alike: they present a green broad emission band from 400 nm to 600 nm centered about 516 nm, this band is due to the intrinsic defects emission of ZnO host. however, in addition to the broad band characteristic of defects in ZnO appear the photoluminescence spectra of the Eu 3+ doped powders: effectively, the sharp peaks in 579, 591, 613, 618, 650 and 770 nm are related to the direct intra-4f transitions in Eu , 1, 2, 3, 4), the most intense emission is associated to the 5 D 0 → 7 F 2 emission in the red spectral region (613 nm) and is due to an allowed electric-dipole transitions with inversion antisymmetry [19], which results in a large transition probability in the crystal field; in our case this emission is split in two components of 613 and 618 nm, theoretically, the 7 F 2 level gives three crystal field levels of A1 and 2E with 3C v symmetry, because A1 and one of two E levels have close energy levels, two emission peaks (A1 and E at 613 and 618 nm) can be overlapped in the PL spectra [34] [35]. The peak at 591 nm is due to the 5 where % is the Eu 3+ ions concentration, the solid curve in Figure 5 represents the fit to the experimental data, the integrated intensity increases as an exponential function as the doping concentration increase which indicates the enhanced energy transfer between the ZnO host and activator Eu 3+ ions.…”