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二维铅笔束扫描质子束斑特性的实验研究。

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

机构信息

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

出版信息

Phys Med Biol. 2013 Sep 7;58(17):6193-204. doi: 10.1088/0031-9155/58/17/6193. Epub 2013 Aug 16.

Abstract

Dose calculations of pencil beam scanning treatment plans rely on the accuracy of proton spot profiles; not only the primary component but also the broad tail components. Four films are placed at several locations in air and multiple depths in Solidwater® for six selected energies. The films used for the primary components are exposed to 50-200 MU to avoid saturation; the films used for the tail components are exposed to 800, 8000 and 80,000 MU. By applying a pair/magnification method and merging these data, dose kernels down to 10(-4) of the central spot dose can be generated. From these kernels one can calculate the dose-per-MU for different field sizes and shapes. Measurements agree within 1% of dose-kernel-based calculations for output versus field size comparisons. Asymmetric, comet-shaped profile tails have a bigger impact at superficial depths and low energies: the output difference between two orientations at the surface of a rectangular field of 40 mm×200 mm is about 2% at the isocentre at 100 MeV. Integration of these dose kernels from 0 to 40 mm radius shows that the charge deficit in the Bragg peak chamber varies <2% from entrance to the end of range for energies <180 MeV, but exceeds 5% at 225 MeV.

摘要

笔形束扫描治疗计划的剂量计算依赖于质子点扩散形状的准确性;不仅需要主要成分,还需要宽的尾部成分。在空气中和 Solidwater®中多个深度的几个位置放置了四个胶片,用于六个选定的能量。用于主要成分的胶片曝光于 50-200MU 以避免饱和;用于尾部成分的胶片曝光于 800、8000 和 80000MU。通过应用一对放大方法并合并这些数据,可以生成低至中央点剂量的 10(-4)的剂量核。从这些核中,可以计算出不同射野大小和形状的每 MU 剂量。对于输出与射野大小的比较,测量值与基于剂量核的计算值在 1%以内一致。不对称的彗星状尾部形状在浅层和低能量时影响更大:在 100MeV 时,40mm×200mm 矩形射野表面两个方向的输出差异在等中心处约为 2%。从 0 到 40mm 半径整合这些剂量核表明,在能量 <180MeV 时,布拉格峰室中的电荷亏损在进入射程末端时变化 <2%,但在 225MeV 时超过 5%。

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