“…where σ is defect capture cross-section with a value of 4 × 10 −13 cm 2 , v th is thermal velocity of the carriers with [6], and N is the concentration of defects, N = kφ and k = βE niel , in which φ is fluence, k is the introduction rate (the number of defects induced by the incident particle), β is a constant coefficient and its value is 3:76 × 10 3 g/MeV/cm 3 [11,26], and E niel (nonionizing energy loss) for 150 keV proton is 0.259 MeV·cm 2 /g [27], so k of 150 keV proton is 974 cm -1 . In fact, irradiation will produce a series of defects with different defect energy levels in the forbidden band, in which deep defect energy levels can function as significant recombination centers.…”