TY - JOUR
T1 - Irradiation-induced defects in Cd 0.9Zn 0.1Te:Al
AU - Nan, Ruihua
AU - Jie, Wanqi
AU - Zha, Gangqiang
AU - Wang, Bei
AU - Xu, Yadong
AU - Yu, Hui
PY - 2012/11
Y1 - 2012/11
N2 - The effects of gamma-irradiation, produced by a 60Co source with a dose of 2.7 kGy, on defect levels in a Cd 0.9Zn 0.1Te:Al (CZT:Al) crystal were investigated by thermally stimulated current spectroscopy. Nine observed defect levels were identified, and the irradiation-induced variations of trap signatures for these levels, i.e., the thermal activation energy, concentration, and capture cross-section, have been evaluated using simultaneous multiple peak analysis. In addition, the dark-current spectra dominated by the deep donor (EDD) level have been certified. By fitting plots of the logarithm of dark current ln(IDC) versus 1/kT, the EDD level is determined to be 0.554 ± 0.001 eV and 0.792 ± 0.004 eV before and after gamma-irradiation, respectively. One month after irradiation, the EDD level moved slightly to 0.782 ± 0.003 eV. This result indicates that the EDD level is closer to the middle of the bandgap of CZT:Al after irradiation, which should be responsible for Fermi-level pinning near the middle of the bandgap, leading to high resistivity. This is consistent with the resistivity variation of CZT:Al at room temperature from the original value of 7.5 9 10 9 ω cm before irradiation to the irradiated value of 5.6 9 10 10 ω cm as determined by current-voltage measurements.
AB - The effects of gamma-irradiation, produced by a 60Co source with a dose of 2.7 kGy, on defect levels in a Cd 0.9Zn 0.1Te:Al (CZT:Al) crystal were investigated by thermally stimulated current spectroscopy. Nine observed defect levels were identified, and the irradiation-induced variations of trap signatures for these levels, i.e., the thermal activation energy, concentration, and capture cross-section, have been evaluated using simultaneous multiple peak analysis. In addition, the dark-current spectra dominated by the deep donor (EDD) level have been certified. By fitting plots of the logarithm of dark current ln(IDC) versus 1/kT, the EDD level is determined to be 0.554 ± 0.001 eV and 0.792 ± 0.004 eV before and after gamma-irradiation, respectively. One month after irradiation, the EDD level moved slightly to 0.782 ± 0.003 eV. This result indicates that the EDD level is closer to the middle of the bandgap of CZT:Al after irradiation, which should be responsible for Fermi-level pinning near the middle of the bandgap, leading to high resistivity. This is consistent with the resistivity variation of CZT:Al at room temperature from the original value of 7.5 9 10 9 ω cm before irradiation to the irradiated value of 5.6 9 10 10 ω cm as determined by current-voltage measurements.
KW - Cd Zn Te
KW - Defects
KW - Irradiation damage
KW - Thermally stimulated current spectroscopy
UR - http://www.scopus.com/inward/record.url?scp=84868597289&partnerID=8YFLogxK
U2 - 10.1007/s11664-012-2204-5
DO - 10.1007/s11664-012-2204-5
M3 - 文章
AN - SCOPUS:84868597289
SN - 0361-5235
VL - 41
SP - 3044
EP - 3049
JO - Journal of Electronic Materials
JF - Journal of Electronic Materials
IS - 11
ER -