Scintillator high-gain avalanche rushing photoconductor active-matrix flat panel imager: Zero-spatial frequency x-ray imaging properties of the solid-state SHARP sensor structure

被引:9
作者
Wronski, M. [2 ]
Zhao, W. [1 ]
Tanioka, K. [3 ]
DeCrescenzo, G. [4 ]
Rowlands, J. A. [4 ]
机构
[1] SUNY Stony Brook, Dept Radiol, Stony Brook, NY 11794 USA
[2] Sunnybrook Hlth Sci Ctr, Dept Radiat Oncol, Toronto, ON M4N 3M5, Canada
[3] Tokyo Denki Univ, Tokyo 1208551, Japan
[4] Thunder Bay Reg Res Inst, Thunder Bay, ON P7A 7T1, Canada
基金
美国国家卫生研究院;
关键词
amorphous selenium; avalanche multiplication gain; flat-panel imager; AMORPHOUS SELENIUM; QUANTUM EFFICIENCY; MULTIPLICATION; CHARGE; SIGNAL; NOISE; PERFORMANCE;
D O I
10.1118/1.4760989
中图分类号
R8 [特种医学]; R445 [影像诊断学];
学科分类号
1002 ; 100207 ; 1009 ;
摘要
Purpose: The authors are investigating the feasibility of a new type of solid-state x-ray imaging sensor with programmable avalanche gain: scintillator high-gain avalanche rushing photoconductor active matrix flat panel imager (SHARP-AMFPI). The purpose of the present work is to investigate the inherent x-ray detection properties of SHARP and demonstrate its wide dynamic range through programmable gain. Methods: A distributed resistive layer (DRL) was developed to maintain stable avalanche gain operation in a solid-state HARP. The signal and noise properties of the HARP-DRL for optical photon detection were investigated as a function of avalanche gain both theoretically and experimentally, and the results were compared with HARP tube (with electron beam readout) used in previous investigations of zero spatial frequency performance of SHARP. For this new investigation, a solid-state SHARP x-ray image sensor was formed by direct optical coupling of the HARP-DRL with a structured cesium iodide (CsI) scintillator. The x-ray sensitivity of this sensor was measured as a function of avalanche gain and the results were compared with the sensitivity of HARP-DRL measured optically. The dynamic range of HARP-DRL with variable avalanche gain was investigated for the entire exposure range encountered in radiography/fluoroscopy (R/F) applications. Results: The signal from HARP-DRL as a function of electric field showed stable avalanche gain, and the noise associated with the avalanche process agrees well with theory and previous measurements from a HARP tube. This result indicates that when coupled with CsI for x-ray detection, the additional noise associated with avalanche gain in HARP-DRL is negligible. The x-ray sensitivity measurements using the SHARP sensor produced identical avalanche gain dependence on electric field as the optical measurements with HARP-DRL. Adjusting the avalanche multiplication gain in HARP-DRL enabled a very wide dynamic range which encompassed all clinically relevant medical x-ray exposures. Conclusions: This work demonstrates that the HARP-DRL sensor enables the practical implementation of a SHARP solid-state x-ray sensor capable of quantum noise limited operation throughout the entire range of clinically relevant x-ray exposures. This is an important step toward the realization of a SHARP-AMFPI x-ray flat-panel imager. (C) 2012 American Association of Physicists in Medicine. [http://dx.doi.org/10.1118/1.4760989]
引用
收藏
页码:7102 / 7109
页数:8
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