Articles you may be interested inDeep-level defects introduced by 1 MeV electron radiation in AlInGaP for multijunction space solar cells J. Appl. Phys. 98, 093701 (2005); 10.1063/1.2115095 Comparison between deep level defects in GaAs induced by gamma, 1 MeV electron, and neutron irradiation Isochronal annealing behavior of deep-level defects in 1 MeV electron irradiated vapor phase epitaxy GaAs was studied through deep level transient spectroscopy measurements. As the annealing temperature was increased, the activation energy of the ELZA trap remained at EC-O.823 eV, whereas the ELZ-B trap (EC-O.843 eV) transformed into a new trap, ELN-1 (Q-O.870 eV), and linally into another new trap, ELN-2 (E,-0.891 eV) before returning to the single EL2-A level at a 270 "C annealing temperature. The EL6 trap (Q-O.335 eV) varied similarly, transforming into EC-O.357 eV (Pl) before staying constant at E,-0.396 eV (ELN3) after a 270 "C! annealing temperature. The capture cross sections of EL2-B and EL6 increased by an order of magnitude during the annealing. These results suggest that the ELZB trap which was split from the EL2 center by the 1 MeV electrons could be related to EL6. Traps El and E2 remain at EC-O.032 eV and EC--O.129 eV, respectively, throughout the annealing, before annihilation at a 290 "C annealing temperature. This result indicates that the atomic structures of El and E2 defects could be related. The EL3 (EC-O.420 eV) is transformed into a new trap, ELN-4 (EC-O.456 eV), and then into &-OS0 eV (P2) during annealing. The free carrier concentration of the irradiated sample increases rapidly with annealing temperature and returns back to the starting free carrier concentration due to the rapid annealing rates of the electron induced defects. 2354