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Improving model–data mismatch for photon‐counting detector model using global and local model parameters

像素 探测器 光子计数 计算机科学 光子 能量(信号处理) 算法 统计 物理 光学 数学 人工智能 电信
作者
Donghyeon Lee,Xiaohui Zhan,Wen-Hsin Tai,Wojciech Zbijewski,Katsuyuki Taguchi
出处
期刊:Medical Physics [Wiley]
卷期号:51 (2): 964-977 被引量:2
标识
DOI:10.1002/mp.16883
摘要

Abstract Background An energy‐discriminating capability of a photon counting detector (PCD) can provide many clinical advantages, but several factors, such as charge sharing (CS) and pulse pileup (PP), degrade the capability by distorting the measured x‐ray spectrum. To fully exploit the merits of PCDs, it is important to characterize the output of PCDs. Previously proposed PCD output models showed decent agreement with physical PCDs; however, there were still scopes to be improved: a global model–data mismatch and pixel‐to‐pixel variations. Purposes In this study, we improve a PCD model by using count‐rate‐dependent model parameters to address the issues and evaluate agreement against physical PCDs. Methods The proposed model is based on the cascaded model, and we made model parameters condition‐dependent and pixel‐specific to deal with the global model–data mismatch and the pixel‐to‐pixel variation. The parameters are determined by a procedure for model parameter estimation with data acquired from different thicknesses of water or aluminum at different x‐ray tube currents. To analyze the effects of having proposed model parameters, we compared three setups of our model: a model with default parameters, a model with global parameters, and a model with global‐and‐local parameters. For experimental validation, we used CdZnTe‐based PCDs, and assessed the performance of the models by calculating the mean absolute percentage errors (MAPEs) between the model outputs and the actual measurements from low count‐rates to high count‐rates, which have deadtime losses of up to 24%. Results The outputs of the proposed model visually matched well with the PCD measurements for all test data. For the test data, the MAPEs averaged over all the bins were 49.2–51.1% for a model with default parameters, 8.0–9.8% for a model with the global parameters, and 1.2–2.7% for a model with the global‐and‐local parameters. Conclusion The proposed model can estimate the outputs of physical PCDs with high accuracy from low to high count‐rates. We expect that our model will be actively utilized in applications where the pixel‐by‐pixel accuracy of a PCD model is important.
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