4.6 Article

Dark Current Modeling for a Polyimide-Amorphous Lead Oxide-Based Direct Conversion X-ray Detector

期刊

SENSORS
卷 22, 期 15, 页码 -

出版社

MDPI
DOI: 10.3390/s22155829

关键词

amorphous lead oxide; blocking layer; mathematical model; dark current; direct conversion; kinetics; polyimide; X-ray detector

资金

  1. Teledyne DALSA
  2. Natural Sciences and Engineering Research Council (NSERC)
  3. Ontario Research Fund-Research Excellence (ORF-RE)
  4. MITACS programs
  5. NSERC

向作者/读者索取更多资源

This study discusses the reduction of dark current in X-ray photoconductors and proposes a theoretical model to describe the electric field-dependent behavior of dark current. The results show that controlling charge injection and reducing the accumulation of trapped holes are crucial in minimizing steady-state dark current. Additionally, the study demonstrates the impact of electric field redistribution on charge collection efficiency and temporal performance.
The reduction of the dark current (DC) to a tolerable level in amorphous selenium (a-Se) X-ray photoconductors was one of the key factors that led to the successful commercialization of a-Se-based direct conversion flat panel X-ray imagers (FPXIs) and their widespread clinical use. Here, we discuss the origin of DC in another X-ray photoconductive structure that utilizes amorphous lead oxide (a-PbO) as an X-ray-to-charge transducer and polyimide (PI) as a blocking layer. The transient DC in a PI/a-PbO detector is measured at different applied electric fields (5-20 V/mu m). The experimental results are used to develop a theoretical model describing the electric field-dependent transient behavior of DC. The results of the DC kinetics modeling show that the DC, shortly after the bias application, is primarily controlled by the injection of holes from the positively biased electrode and gradually decays with time to a steady-state value. DC decays by the overarching mechanism of an electric field redistribution, caused by the accumulation of trapped holes in deep localized states within the bulk of PI. Thermal generation and subsequent multiple-trapping (MT) controlled transport of holes within the a-PbO layer governs the steady-state value at all the applied fields investigated here, except for the largest applied field of 20 V/mu m. This suggests that a thicker layer of PI would be more optimal to suppress DC in the PI/a-PbO detector presented here. The model can be used to find an approximate optimal thickness of PI for future iterations of PI/a-PbO detectors without the need for time and labor-intensive experimental trial and error. In addition, we show that accounting for the field-induced charge carrier release from traps, enhanced by charge hopping transitions between the traps, yields an excellent fit between the experimental and simulated results, thus, clarifying the dynamic process of reaching a steady-state occupancy level of the deep localized states in the PI. Practically, the electric field redistribution causes the internal field to increase in magnitude in the a-PbO layer, thus improving charge collection efficiency and temporal performance over time, as confirmed by experimental results. The electric field redistribution can be implemented as a warm-up time for a-PbO-based detectors.

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