TY - JOUR
T1 - Detection of charged particles and X-rays by scintillator layers coupled to amorphous silicon photodiode arrays
AU - Jing, T.
AU - Goodman, C. A.
AU - Drewery, J.
AU - Cho, G.
AU - Hong, W. S.
AU - Lee, H.
AU - Kaplan, S. N.
AU - Perez-Mendez, V.
AU - Wildermuth, D.
PY - 1996/1/11
Y1 - 1996/1/11
N2 - Hydrogenated amorphous silicon (a-Si:H) p-i-n diodes with transparent metallic contacts are shown to be suitable for detecting charged particles, electrons, and X-rays. When coupled to a suitable scintillator using CsI(Tl) as the scintillator we show a capability to detect minimum ionizing particles with S/N ∼20. We demonstrate such an arrangement by operating a p-i-n diode in photovolaic mode (reverse bias). Moreover, we show that a p-i-n diode can also work as a photoconductor under forward bias and produces a gain yield of 3-8 higher light sensitivity for shaping times of 1 μs. n-i-n devices have similar optical gain as the p-i-n photoconductor for short integrating times (<10 μs). However, n-i-n devices exhibit much higher gain for a long term integration (10 ms) than the p-i-n ones. High sensitivity photosensors are very desirable for X-ray medical imaging because radiation exposure dose can be reduced significantly. The scintillator CsI layers we made have higher spatial resolution than the Kodak commercial scintillator screens due to their internal columnar structure which can collimate the scintitlator light. Evaporated CsI layers are shown to be more resistant to radiation damage than the crystalline bulk CsI(Tl).
AB - Hydrogenated amorphous silicon (a-Si:H) p-i-n diodes with transparent metallic contacts are shown to be suitable for detecting charged particles, electrons, and X-rays. When coupled to a suitable scintillator using CsI(Tl) as the scintillator we show a capability to detect minimum ionizing particles with S/N ∼20. We demonstrate such an arrangement by operating a p-i-n diode in photovolaic mode (reverse bias). Moreover, we show that a p-i-n diode can also work as a photoconductor under forward bias and produces a gain yield of 3-8 higher light sensitivity for shaping times of 1 μs. n-i-n devices have similar optical gain as the p-i-n photoconductor for short integrating times (<10 μs). However, n-i-n devices exhibit much higher gain for a long term integration (10 ms) than the p-i-n ones. High sensitivity photosensors are very desirable for X-ray medical imaging because radiation exposure dose can be reduced significantly. The scintillator CsI layers we made have higher spatial resolution than the Kodak commercial scintillator screens due to their internal columnar structure which can collimate the scintitlator light. Evaporated CsI layers are shown to be more resistant to radiation damage than the crystalline bulk CsI(Tl).
UR - http://www.scopus.com/inward/record.url?scp=4244156134&partnerID=8YFLogxK
U2 - 10.1016/0168-9002(95)00602-8
DO - 10.1016/0168-9002(95)00602-8
M3 - Article
AN - SCOPUS:4244156134
SN - 0168-9002
VL - 368
SP - 757
EP - 764
JO - Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
JF - Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
IS - 3
ER -