Stanescu T, Jaffray D
Princess Margaret Cancer Centre, University Health Network, Toronto, Ontario M5G 2M9, Canada and Department of Radiation Oncology, University of Toronto, 610 University Avenue, Toronto, Ontario M5G 2M9, Canada.
Med Phys. 2016 Mar;43(3):1550-62. doi: 10.1118/1.4941958.
Magnetic resonance (MR) images are affected by geometric distortions due to the specifics of the MR scanner and patient anatomy. Quantifying the distortions associated with mobile tumors is particularly challenging due to real anatomical changes in the tumor's volume, shape, and relative location within the MR imaging volume. In this study, the authors investigate the 4D composite distortion field, which combines the effects of the susceptibility-induced and system-related distortion fields, experienced by mobile lung tumors.
The susceptibility (χ) effects were numerically simulated for two specific scenarios: (a) a full motion cycle of a lung tumor due to breathing as depicted on ten phases of a 4D CBCT data set and (b) varying the tumor size and location in lung tissue via a synthetically generated sphere with variable diameter (4-80 mm). The χ simulation procedure relied on the segmentation and generation of 3D susceptibility (χ) masks and computation of the magnetic field by means of finite difference methods. A system-related distortion field, determined with a phantom and image processing algorithm, was used as a reference. The 4D composite distortion field was generated as the vector summation of the χ-induced and system-related fields. The analysis was performed for two orientations of the main magnetic field (B0), which correspond to several MRIgRT system configurations. Specifically, B0 was set along the z-axis as in the case of a cylindrical-bore scanner and in the (x,y)-plane as for a biplanar MR. Computations were also performed for a full revolution at 15° increments in the case of a rotating biplanar magnet. Histograms and metrics such as maximum, mean, and range were used to evaluate the characteristics of the 4D distortion field.
The χ-induced field depends on the change in volume and shape of the moving tumor as well as the local surrounding anatomy. In the case of system-related distortions, the tumor experiences increased field perturbations as it moves further away from the MR isocenter. For a mobile lung tumor, the 4D composite field, corresponding to a 1.5 T field and a readout gradient of 5 mT/m, amounts to 3.0 and 2.8 mm for the MRIgRT system designs featuring B0 oriented along the z-axis (cylindrical-bore scanner) and in the (x,y)-plane (biplanar scanner), respectively. For a rotating biplanar scanner, the composite distortion field varied nonlinearly with the rotation angle. Overall, the dominant contribution to the composite field was from the system-related distortion field. The tumor centroid experienced a systematic shift of 2 mm and showed a negligible perturbation for different B0 values. The dependency on the tumor size was also investigated, namely the max values varied from 1.2 to 2.5 mm for spherical volumes with a diameter between 4 and 80 mm.
The composite distortion field requires adequate quantification for lung radiation therapy applications such as treatment planning, pretreatment patient setup verification, and real-time treatment delivery guidance. For certain scenarios such as small tumor volumes, the spatial distortions may be corrected by applying systematic shifts derived from a single tumor motion phase. In the case of high readout gradients common to fast imaging applications, the χ distortions were found to be less than 1 mm irrespective of scanner configuration.
由于磁共振(MR)扫描仪和患者解剖结构的特殊性,MR图像会受到几何失真的影响。由于肿瘤在MR成像体积内的体积、形状和相对位置发生实际解剖学变化,对与移动性肿瘤相关的失真进行量化尤其具有挑战性。在本研究中,作者研究了移动性肺肿瘤所经历的4D复合失真场,该场结合了由磁化率诱导和系统相关失真场的影响。
针对两种特定情况对磁化率(χ)效应进行了数值模拟:(a)如4D CBCT数据集的十个阶段所示,肺肿瘤因呼吸而产生的完整运动周期;(b)通过直径可变(4 - 80 mm)的合成球体改变肿瘤在肺组织中的大小和位置。χ模拟过程依赖于3D磁化率(χ)掩码的分割和生成以及通过有限差分法计算磁场。使用体模和图像处理算法确定的系统相关失真场作为参考。4D复合失真场通过χ诱导场和系统相关场的矢量求和生成。针对主磁场(B0)的两个方向进行了分析,这对应于几种MRIgRT系统配置。具体而言,B0如圆柱形孔扫描仪那样沿z轴设置,以及如双平面MR那样在(x,y)平面设置。对于旋转双平面磁体,还以15°增量进行了一整圈的计算。使用直方图和诸如最大值、平均值和范围等指标来评估4D失真场的特征。
χ诱导场取决于移动肿瘤的体积和形状变化以及局部周围解剖结构。在系统相关失真的情况下,肿瘤离MR等中心越远,经历的场扰动就越大。对于移动性肺肿瘤,对于B0沿z轴(圆柱形孔扫描仪)和在(x,y)平面(双平面扫描仪)取向的MRIgRT系统设计,对应于1.5 T场和5 mT/m读出梯度的4D复合场分别为3.0和2.8 mm。对于旋转双平面扫描仪,复合失真场随旋转角度呈非线性变化。总体而言,对复合场的主要贡献来自系统相关失真场。肿瘤质心经历了2 mm的系统性偏移,并且对于不同的B0值显示出可忽略不计的扰动。还研究了对肿瘤大小的依赖性,即对于直径在4至