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一种实用的方法来估计无限积分长度的加权 CT 剂量指数。

A practical approach to estimate the weighted CT dose index over an infinite integration length.

机构信息

Division of Diagnostic Imaging Physics, Department of Radiology, Massachusetts General Hospital, Boston, MA 02114, USA.

出版信息

Phys Med Biol. 2011 Sep 21;56(18):5789-803. doi: 10.1088/0031-9155/56/18/002. Epub 2011 Aug 16.

Abstract

The CT scanner-displayed radiation dose information is based on CT dose index (CTDI) over an integration length of 100 mm (CTDI(100)), which is lower than the CTDI over an infinite integration length (CTDI(∞)). In an adult or a pediatric body CT scan, the limiting equilibrium dose can be established near the central scan plane, and CTDI(∞) more closely indicates the accumulated dose than CTDI(100). The aim of this study was to (a) evaluate CTDI efficiencies, ϵ(CTDI(100)) = CTDI(100)/CTDI(∞), for a multi-detector CT (MDCT) scanner, (b) examine the dependences of ϵ(CTDI(100)) on kV, beam width, phantom diameter, phantom length and position in phantom and (c) investigate how to estimate CTDI(∞) based on the CT scanner-displayed information. We performed a comprehensive Geant4-based simulation study of a clinical CT scanner, and calculated ϵ(CTDI(100)) for a range of parameters. The results were compared with the ϵ(CTDI(100)) data of previous studies. Differences in the ϵ(CTDI(100)) values of these studies were assessed. A broad analysis of the ϵ(CTDI(100)) variations with the above-mentioned parameters was presented. Based on the results, we proposed a practical approach to obtain the weighted CTDI(∞) using the CT scanner-displayed information. A reference combination of 120 kV and a beam width close to 20 mm can be selected to determine the efficiencies of the weighted CTDI by using either phantom measurements or computer simulations. The results can be applied to estimate the weighted CTDI(∞) for 80-140 kV and the beam widths within 40 mm. Errors in the weighted CTDI(∞) due to the variations of kV and beam width can be 5% or less for the MDCT scanners.

摘要

CT 扫描仪显示的辐射剂量信息基于 100mm 积分长度的 CT 剂量指数(CTDI(100)),低于无限积分长度的 CTDI(CTDI(∞))。在成人或儿科体部 CT 扫描中,可以在中央扫描平面附近建立限制平衡剂量,而 CTDI(∞)比 CTDI(100)更能准确地反映累积剂量。本研究旨在:(a) 评估多探测器 CT(MDCT)扫描仪的 CTDI 效率,ϵ(CTDI(100))=CTDI(100)/CTDI(∞);(b) 考察 ϵ(CTDI(100))对 kV、射束宽度、模体直径、模体长度和模体位置的依赖性;(c) 研究如何根据 CT 扫描仪显示的信息估算 CTDI(∞)。我们对临床 CT 扫描仪进行了全面的 Geant4 模拟研究,计算了一系列参数下的 ϵ(CTDI(100))。并将结果与之前研究中的 ϵ(CTDI(100))数据进行了比较。评估了这些研究中 ϵ(CTDI(100))值的差异。提出了一种基于上述参数的 ϵ(CTDI(100))变化的广泛分析方法。根据结果,我们提出了一种使用 CT 扫描仪显示信息获得加权 CTDI(∞)的实用方法。可以选择 120kV 的参考组合和接近 20mm 的射束宽度,使用模体测量或计算机模拟来确定加权 CTDI 的效率。该结果可应用于估算 80-140kV 范围内和 40mm 内的射束宽度的加权 CTDI(∞)。对于 MDCT 扫描仪,kV 和射束宽度变化引起的加权 CTDI(∞)误差可控制在 5%以内。

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