Abstract

In the last ten to fifteen years there has been much research in using amorphous and polycrystalline semiconductors as x-ray photoconductors in various x-ray image sensor applications, most notably in flat panel x-ray imagers (FPXIs). We first outline the essential requirements for an ideal large area photoconductor for use in a FPXI, and discuss how some of the current amorphous and polycrystalline semiconductors fulfill these requirements. At present, only stabilized amorphous selenium (doped and alloyed a-Se) has been commercialized, and FPXIs based on a-Se are particularly suitable for mammography, operating at the ideal limit of high detective quantum efficiency (DQE). Further, these FPXIs can also be used in real-time, and have already been used in such applications as tomosynthesis. We discuss some of the important attributes of amorphous and polycrystalline x-ray photoconductors such as their large area deposition ability, charge collection efficiency, x-ray sensitivity, DQE, modulation transfer function (MTF) and the importance of the dark current. We show the importance of charge trapping in limiting not only the sensitivity but also the resolution of these detectors. Limitations on the maximum acceptable dark current and the corresponding charge collection efficiency jointly impose a practical constraint that many photoconductors fail to satisfy. We discuss the case of a-Se in which the dark current was brought down by three orders of magnitude by the use of special blocking layers to satisfy the dark current constraint. There are also a number of polycrystalline photoconductors, HgI2 and PbO being good examples, that show potential for commercialization in the same way that multilayer stabilized a-Se x-ray photoconductors were developed for commercial applications. We highlight the unique nature of avalanche multiplication in a-Se and how it has led to the development of the commercial HARP video-tube. An all solid state version of the HARP has been recently demonstrated with excellent avalanche gains; the latter is expected to lead to a number of novel imaging device applications that would be quantum noise limited. While passive pixel sensors use one TFT (thin film transistor) as a switch at the pixel, active pixel sensors (APSs) have two or more transistors and provide gain at the pixel level. The advantages of APS based x-ray imagers are also discussed with examples.

Highlights

  • Direct Conversion Flat Panel X-Ray ImagersFlat panel x-ray imagers (FPXIs) are widely used in digital x-ray imaging with applications in medical, security and industrial imaging

  • The reader should note that the majority of the work relating the x-ray image detector performance to charge carrier deep trapping effects was done in Canada

  • 5.45 10 13 e where the first term gives the incident photon fluence per unit Roentgen, the second is the attenuated fraction of the incident photons, that is, the quantum efficiency, the third is the number of electron hole pairs (EHPs) created per absorbed radiation energy, and the fourth is the fraction of those charges that are collected

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Summary

Introduction

Flat panel x-ray imagers (FPXIs) are widely used in digital x-ray imaging with applications in medical, security and industrial imaging. In addition to a-Se, there have been a number of other photoconductors, such as polycrystalline layers of TlBr [46,47], PbI2 [48,49], HgI2 [50,51,52,53,54,55,56], CdZnTe [57,58] and PbO [59,60], that have been investigated and some of these, in particular HgI2 and PbO, have shown potential for use in commercial FPXI applications Most of these photoconductors to date either suffer from possessing too large a dark current or not having sufficient charge collection efficiency. The present review only considers potential amorphous or polycrystalline photoconductors that can be or could be deposited on a large TFT-AMA substrate to fabricate a FPXI that would be useful in x-ray imaging such as radiography or fluoroscopy. The main drawbacks of photoconductor-coated imaging chips are their limited area, that is, field of view requiring tiling for large area applications, and their cost

Potential Large Area Photoconductors
Quantum Efficiency AQ
Dark Current
Charge Collection Efficiency CCE
X-Ray Damage and Fatigue
Large Area Fabrication
Charge Carrier Transport and Imager Performance
X-Ray Sensitivity
Detective Quantum Efficiency
X-Ray Photoconductors with Avalanche Gain and Imaging Applications
Findings
Active Pixel Sensor Based X-Ray Imagers
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