“…Among the multitude of radiation induced electrically active defects only some proved to have a direct impact on the "macroscopic" behavior of the sensors operating at ambient temperatures. These point-or extended-defects are labeled in the literature as: I p -a deep acceptor strongly generated in oxygen lean, standard float-zone material (STFZ) [22][23][24] and BD-a bistable thermal donor (TDD2) 24,26,27 strongly generated in oxygen rich float-zone material (DOFZ), both associated with point defects that are stable at room temperature and determining the N eff in silicon diodes irradiated with Co 60 g-rays; E(30K)-a shallow donor contributing to the a) R. Radu beneficial annealing after hadron irradiation, strongly generated in diodes irradiated with charged particles; 10,29 H(116K), H(140K), H(152K)-cluster-related hole traps with enhanced field emission (acceptors in the lower part of the Si bandgap), contributing fully with their concentration to N eff and causing the long term annealing effects (reverse annealing) in hadron irradiated silicon diodes; 10,29 the bistable E4 and E5 energy levels-identified with the double and single acceptor charge state of the V 3 defect in a configuration part of a hexagonal ring (PHR), respectively, [30][31][32][33] a defect contributing to the magnitude of the leakage current in the Si sensors and bipolar transistors upon irradiation with high energy particles. 28,31 The most important characteristics of these defects, including some features resulted from the present work, are summarized in Table I.…”