Maeda Koji, Matsumoto Masao, Taniguchi Akita, Kanamori Hitoshi
Department of Clinical Radiology, Faculty of Health Sciences, Hiroshima International University, 555-36 Gakuendai, Kurose-machi, Kamo-gun, Hiroshima-pref. 724-0695, Jap.
Igaku Butsuri. 2004;24(2):49-60.
The purpose of this study is to measure diagnostic x-ray spectra using a high resolution Schottky CdTe detector (TOYO MEDIC RAMTEC 413A) and to determine the best response function of CdTe detector for correcting the measured spectra with using a rise time discrimination (RTD) circuit to primary x-ray spectra. Since the measured spectra were distorted by the response of CdTe detector and did not present the true photon spectra, the correction by the stripping procedure was applied. The response function of CdTe detector has been determined by using Monte Carlo simulation method for calculating the photon interaction (K-escape, coherent scattering and Compton scattering) and incomplete charge collection by trapping of hole and use of RTD circuit. This simulation performed with various important factors (mean path length lambda(h) of hole and weight factor W(q) of incomplete charge collection) for finding the best response function. The photon spectra corrected with those various response functions were compared with the corrected photon spectra measured using a high purity Ge (HP-Ge) detector (PRINCETON GAMMA-TECH NIGP1013345), and the Al-attenuation curves calculated from corrected spectra and measured using the HP-Ge detector were compared. The best-fitted response function was determined, and the attenuation curves calculated from the spectra corrected with this response function were agreed with that measured using the HP-Ge detector within maximum error 0.03 of the attenuation rate and 5.0 % of the half value layer.
本研究的目的是使用高分辨率肖特基碲化镉探测器(东洋医疗RAMTEC 413A)测量诊断X射线光谱,并确定碲化镉探测器对于使用上升时间鉴别(RTD)电路对初级X射线光谱测量光谱进行校正的最佳响应函数。由于测量的光谱因碲化镉探测器的响应而失真,未呈现真实的光子光谱,因此应用了剥离程序进行校正。碲化镉探测器的响应函数已通过蒙特卡罗模拟方法确定,用于计算光子相互作用(K逃逸、相干散射和康普顿散射)以及通过空穴俘获和使用RTD电路导致的不完全电荷收集。该模拟针对各种重要因素(空穴的平均路径长度λ(h)和不完全电荷收集的权重因子W(q))进行执行,以找到最佳响应函数。将用这些不同响应函数校正后的光子光谱与使用高纯锗(HP-Ge)探测器(普林斯顿伽马技术NIGP1013345)测量的校正光子光谱进行比较,并将根据校正光谱计算并使用HP-Ge探测器测量的铝衰减曲线进行比较。确定了最佳拟合响应函数,并且由用该响应函数校正的光谱计算出的衰减曲线与使用HP-Ge探测器测量出的衰减曲线在衰减率的最大误差0.03和半值层的5.0%范围内一致。