Chow James C L, Grigorov Grigor N, Jiang Runqing
Department of Radiation Oncology, University of Toronto and Radiation Medicine Program, Princess Margaret Hospital, University Health Network, 610 University Avenue, Toronto, ON N2G 1G3, Canada.
Med Phys. 2006 Dec;33(12):4606-13. doi: 10.1118/1.2388571.
Using a Varian 21 EX linear accelerator with a multileaf collimator (MLC) of 120 leaves, the penumbra regions of beam profiles within an irregular multileaf collimated fields were studied. MLC fields with different leaf stepping angles from 21.8 degrees to 68.2 degrees were used. Beam profiles in different directions: (1) along the cross-line and in-line axis, (2) along the leaf stepping edges of the field, and (3) parallel to the stepping edges but in the middle of the field, were measured and calculated using Kodak XV radiographic film and Pinnacle3 treatment planning system version 7.4f. These beam profiles were measured and calculated at source to axis distance= 100 cm with 5 cm of solid water slab on top. On the one hand, for both cross-line and in-line beam profiles, the penumbra widths of 20%-80% did not vary with the leaf stepping angles and were about 0.4 cm. On the other hand, the penumbra widths of 10%-90% of the above two profiles varied with the stepping angles and had maximum widths of about 1.9 cm (cross-line) and 1.65 cm (in-line) for stepping angles of 38.7 degrees and 51.3 degrees , respectively. For profiles crossing the "rippled" stepping edges of the field, the penumbra widths (10%-90%) at the regions between two opposite leaves (i.e., profile end at the Y1/Y2 jaw position) decreased with the stepping angles. At the penumbra regions between two leaf edges with the tongue-and-groove structure of the same bank (i.e., profile end at the X1/X2 jaw position), the penumbra widths increased with the stepping angles. When the penumbra widths were measured between two opposite leaf edges and at corners between two leaves, the widths first decreased with the stepping angles and then increased beyond the minimum width point at stepping angle of 45 degrees. The penumbra width (10%-90%) measured at the leaf edge was larger than that at the corner. For the beam profiles calculated using Pinnacle3, it is found that the results agreed well with the measurements along the cross-line and in-line axis, while there was a deviation for the profiles along the leaf stepping edge of the field compared to the film measurements. The measured results in this study can help us to understand the dosimetric effect of the leaf stepping (due to finite leaf width), tongue-and-groove and rounded leaf end structure in the penumbra region of an irregular MLC field. A more dedicated penumbra model can be developed for the treatment planning system.
使用配备120叶多叶准直器(MLC)的瓦里安21EX直线加速器,研究了不规则多叶准直野内射束轮廓的半影区。使用了叶步角从21.8度到68.2度不等的MLC野。在不同方向上的射束轮廓:(1)沿着交叉线和线束轴,(2)沿着野的叶步边缘,以及(3)平行于步边缘但在野的中间,使用柯达XV射线照相胶片和Pinnacle3治疗计划系统版本7.4f进行测量和计算。这些射束轮廓在源轴距 = 100 cm且顶部有5 cm固体水模体的条件下进行测量和计算。一方面,对于交叉线和线束射束轮廓,20%-80%的半影宽度不随叶步角变化,约为0.4 cm。另一方面,上述两种轮廓10%-90%的半影宽度随步角变化,对于步角分别为38.7度和51.3度时,交叉线方向的最大宽度约为1.9 cm,线束方向的最大宽度约为1.65 cm。对于穿过野“波纹状”步边缘的轮廓,在两个相对叶片之间的区域(即Y1/Y2光阑位置处的轮廓末端)的半影宽度(10%-90%)随步角减小。在同一排具有榫槽结构的两个叶边缘之间的半影区(即X1/X2光阑位置处的轮廓末端),半影宽度随步角增加。当在两个相对叶边缘之间以及两个叶片之间的角落测量半影宽度时,宽度首先随步角减小,然后在步角为45度时超过最小宽度点后增加。在叶边缘测量的半影宽度(10%-90%)大于在角落处的半影宽度。对于使用Pinnacle3计算的射束轮廓,发现沿交叉线和线束轴的结果与测量结果吻合良好,而与胶片测量相比,沿野叶步边缘的轮廓存在偏差。本研究中的测量结果有助于我们理解叶步(由于叶片有限宽度)、榫槽和圆形叶端结构在不规则MLC野半影区的剂量学效应。可以为治疗计划系统开发更专用的半影模型。