Helsinki University Central Hospital Ltd, HUS, Finland.
Med Phys. 2013 Jan;40(1):011701. doi: 10.1118/1.4769407.
Magnetic resonance (MR) images are used increasingly in external radiotherapy target delineation because of their superior soft tissue contrast compared to computed tomography (CT) images. Nevertheless, radiotherapy treatment planning has traditionally been based on the use of CT images, due to the restrictive features of MR images such as lack of electron density information. This research aimed to measure absorbed radiation doses in material behind different bone parts, and to evaluate dose calculation errors in two pseudo-CT images; first, by assuming a single electron density value for the bones, and second, by converting the electron density values inside bones from T(1)∕T(2)∗-weighted MR image intensity values.
A dedicated phantom was constructed using fresh deer bones and gelatine. The effect of different bone parts to the absorbed dose behind them was investigated with a single open field at 6 and 15 MV, and measuring clinically detectable dose deviations by an ionization chamber matrix. Dose calculation deviations in a conversion-based pseudo-CT image and in a bulk density pseudo-CT image, where the relative electron density to water for the bones was set as 1.3, were quantified by comparing the calculation results with those obtained in a standard CT image by superposition and Monte Carlo algorithms.
The calculations revealed that the applied bulk density pseudo-CT image causes deviations up to 2.7% (6 MV) and 2.0% (15 MV) to the dose behind the examined bones. The corresponding values in the conversion-based pseudo-CT image were 1.3% (6 MV) and 1.0% (15 MV). The examinations illustrated that the representation of the heterogeneous femoral bone (cortex denser compared to core) by using a bulk density for the whole bone causes dose deviations up to 2% both behind the bone edge and the middle part of the bone (diameter <2.5 cm), but in the opposite directions. The measured doses and the calculated ones in the standard CT image were within 0.4% (through gelatine only) and 0.9% (behind bones).
This study indicates that the decrease in absorbed dose is not dependent on the bone diameter with all types of bones. Thus, performing dose calculation in a pseudo-CT image by assuming a single electron density value for the bones can lead to a substantial misrepresentation of the dose distribution profile. This work showed that dose calculation accuracy can be improved by using a pseudo-CT image in which the electron density values have been converted from the MR image intensity values inside bones.
与计算机断层扫描(CT)图像相比,磁共振(MR)图像具有优越的软组织对比度,因此越来越多地用于外部放射治疗靶区勾画。然而,由于 MR 图像缺乏电子密度信息等限制因素,放射治疗计划传统上一直基于 CT 图像。本研究旨在测量不同骨部位后面的吸收剂量,并评估两种伪 CT 图像中的剂量计算误差;首先,假设骨骼的单一电子密度值,其次,通过将骨骼内的电子密度值从 T(1)∕T(2)∗-加权 MR 图像强度值转换。
使用新鲜鹿骨和明胶构建专用体模。使用单开野在 6 和 15 MV 下研究不同骨部位对其后吸收剂量的影响,并通过电离室矩阵测量临床可检测剂量偏差。通过将计算结果与标准 CT 图像的叠加和蒙特卡罗算法的计算结果进行比较,量化基于转换的伪 CT 图像和体密度伪 CT 图像中的剂量计算偏差,其中骨骼的相对电子密度与水设定为 1.3。
计算结果表明,应用的体密度伪 CT 图像导致检查骨骼后面的剂量偏差高达 2.7%(6 MV)和 2.0%(15 MV)。基于转换的伪 CT 图像中的相应值分别为 1.3%(6 MV)和 1.0%(15 MV)。检查结果表明,使用整个骨骼的体密度表示不均匀的股骨(皮质比核心致密)会导致骨骼边缘和骨骼中部(直径<2.5cm)的剂量偏差高达 2%,但方向相反。通过凝胶仅测量的剂量和标准 CT 图像中的计算剂量在 0.4%(通过凝胶)和 0.9%(在骨骼后面)范围内。
本研究表明,吸收剂量的降低与所有类型的骨骼的骨直径无关。因此,通过对骨骼假设单一电子密度值在伪 CT 图像中进行剂量计算可能会导致剂量分布曲线的严重失真。这项工作表明,通过使用将骨骼内的电子密度值从 MR 图像强度值转换而来的伪 CT 图像,可以提高剂量计算的准确性。