TY - JOUR
T1 - Electrically active defects in neutron-irradiated HPSI 4H-SiC X-ray detectors investigated by ZB-TSC technique
AU - Raja, P. Vigneshwara
AU - Murty, N. V.L.Narasimha
N1 - Publisher Copyright:
© 1963-2012 IEEE.
PY - 2017/8
Y1 - 2017/8
N2 - Electrically active defects in high-purity semi-insulating (HPSI) 4H-silicon carbide (4H-SiC) X-ray detectors have been characterized before and after neutron irradiation by zero-bias thermally stimulated current (ZB-TSC) and high-temperature resistivity measurements. The ZB-TSC measurements prior to irradiation reveal nine hole traps in the energy range of 0.22-1.16 eV and two electron traps at Ec-0.35 eV and Ec-0.44 eV. For the same case, high-temperature resistivity measurements yield thermal activation energy in the range of 1-1.3 eV. It is considered that the hole traps at Ev+ 0.83 eV and Ev+ 1.16 eV along with defects located near the activation energies are possibly responsible for the substrate compensation. A poor resolution of 11.8-keV full-width at half-maximum (at 40 keV of 152Eu) with un-irradiated HPSI 4H-SiC detectors is attributed to the charge trapping and polarization effects. After neutron irradiation at the fluence of 10^{11} n/cm2, seven new traps ( Ev+ 0.68 eV, Ev + 1.08 eV, Ev + 1.22 eV, Ec-0.72 eV, Ec- 0.9 eV, Ec- 1.04 eV, and Ec- 1.1 eV) are identified with no significant changes in the activation energies. This indicates that the substrate resistivity is unaffected by the neutron-irradiation-induced defects. No considerable changes in the X-ray spectral response are noted at 1011} n/cm2.
AB - Electrically active defects in high-purity semi-insulating (HPSI) 4H-silicon carbide (4H-SiC) X-ray detectors have been characterized before and after neutron irradiation by zero-bias thermally stimulated current (ZB-TSC) and high-temperature resistivity measurements. The ZB-TSC measurements prior to irradiation reveal nine hole traps in the energy range of 0.22-1.16 eV and two electron traps at Ec-0.35 eV and Ec-0.44 eV. For the same case, high-temperature resistivity measurements yield thermal activation energy in the range of 1-1.3 eV. It is considered that the hole traps at Ev+ 0.83 eV and Ev+ 1.16 eV along with defects located near the activation energies are possibly responsible for the substrate compensation. A poor resolution of 11.8-keV full-width at half-maximum (at 40 keV of 152Eu) with un-irradiated HPSI 4H-SiC detectors is attributed to the charge trapping and polarization effects. After neutron irradiation at the fluence of 10^{11} n/cm2, seven new traps ( Ev+ 0.68 eV, Ev + 1.08 eV, Ev + 1.22 eV, Ec-0.72 eV, Ec- 0.9 eV, Ec- 1.04 eV, and Ec- 1.1 eV) are identified with no significant changes in the activation energies. This indicates that the substrate resistivity is unaffected by the neutron-irradiation-induced defects. No considerable changes in the X-ray spectral response are noted at 1011} n/cm2.
KW - Defects
KW - X-ray detector
KW - high-purity semi-insulating (HPSI) 4H-silicon carbide (4H-SiC)
KW - radiation damage
KW - thermally stimulated current (TSC)
UR - http://www.scopus.com/inward/record.url?scp=85023754697&partnerID=8YFLogxK
U2 - 10.1109/TNS.2017.2720192
DO - 10.1109/TNS.2017.2720192
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AN - SCOPUS:85023754697
SN - 0018-9499
VL - 64
SP - 2377
EP - 2385
JO - IEEE Transactions on Nuclear Science
JF - IEEE Transactions on Nuclear Science
IS - 8
M1 - 7959206
ER -