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二维点扫描束流喷嘴质子束流的实验特性分析。

Experimental characterization of two-dimensional spot profiles for two proton pencil beam scanning nozzles.

机构信息

Department of Radiation Oncology, University of Pennsylvania, 3400 Civic Blvd, Philadelphia, PA 19104, USA.

出版信息

Phys Med Biol. 2014 Jan 20;59(2):493-504. doi: 10.1088/0031-9155/59/2/493. Epub 2013 Dec 30.

Abstract

Dose calculation for pencil beam scanning proton therapy requires accurate measurement of the broad tails of the proton spot profiles for every nozzle in clinical use. By applying a pair/magnification method and merging film data, 200 mm × 240 mm dose kernels extending to 10(-4) of the central spot dose are generated for six selected energies of the IBA dedicated and universal nozzles (DN and UN). One-dimensional, circular profiles up to 100 mm in radius are generated from the asymmetric profiles to facilitate spot profile comparison. For the highest energy, 225 MeV, the output of both the DN and the UN for field sizes from 40 to 200 mm increases in parallel, slowest at the surface (∼1%) and fastest at a depth of 150 mm (∼9%). In contrast, at the lowest energy, 100 MeV, the output of the DN across the same range of field sizes increases 3-4% versus 6-7% for the UN throughout all the depths. The charge deficits in the measured depth-dose of Bragg peaks are similar between the UN and the DN. At 100 MeV, the field size factor difference at the surface between two orientations of a rectangular 40 mm × 200 mm field is 1.4% at isocentre for the DN versus 2% for the UN. Though the one-dimensional distributions are similar for the primary and tail components at different positions, the primary components of the DN spots are more elliptical 270 mm upstream than at isocentre.

摘要

笔形束扫描质子治疗的剂量计算需要准确测量每个临床使用的喷嘴的质子束斑轮廓的宽尾。通过应用一对/放大方法和合并胶片数据,为六个选定的 IBA 专用和通用喷嘴(DN 和 UN)能量生成了扩展到中央光斑剂量的 10(-4)的 200mm×240mm 剂量核。从不对称轮廓生成一维、圆形轮廓,半径可达 100mm,以方便光斑轮廓比较。对于最高能量 225MeV,DN 和 UN 的输出对于 40 至 200mm 的射野大小呈平行增加,在表面最慢(约 1%),在 150mm 深度最快(约 9%)。相比之下,在最低能量 100MeV 下,DN 在相同的射野大小范围内的输出增加了 3-4%,而 UN 在所有深度的输出增加了 6-7%。在 Bragg 峰的测量深度剂量中,UN 和 DN 之间的电荷不足相似。在 100MeV 时,两个方向的 40mm×200mm 矩形射野在等中心处的表面场大小因子差为 DN 为 1.4%,UN 为 2%。尽管在不同位置,一维分布对于主成分和尾部成分相似,但 DN 光斑的主成分在 270mm 上游比在等中心更椭圆。

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