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遮挡块对12兆电子伏和14兆电子伏电子束的输出剂量、平均能量和百分深度剂量的影响。

The effects of cutouts on output, mean energy and percentage depth dose of 12 and 14 MeV electrons.

作者信息

Khaledy Navid, Arbabi Azim, Sardari Dariush

机构信息

Young Researchers Club, Science and Research Branch, Islamic Azad University, Tehran, Iran.

出版信息

J Med Phys. 2011 Oct;36(4):213-9. doi: 10.4103/0971-6203.89970.

Abstract

Electron field-shaping cerrobend cutouts on the linear accelerator applicator have some effects on the output and percentage depth dose. These effects which arise from the lateral scatter nonequilibrium are particularly evident in higher energies and in cutouts with smaller radius. Dose measurements for circular, square, and triangular cutouts as well as open field was performed in a 10 × 10 cm applicator, using plane parallel type ion chamber with a 100 cm source surface distance. The Percentage Depth Doses curves were drawn and the outputs were measured for each of these cutouts. The output factors, normalized to open 10 × 10 cm field, varied between 0.891 and 0.996 depending on the energy, cutout shape, and cavity area. With the use of cutouts, R(100) shifted toward the surface. The shifts ranged from 9 to 0 mm and from 13 to 0 mm for 12 and 14 MeV, respectively, depending on the shape and cavity area. For R(90), R(80), and R(50) the ranges for observed shifts narrowed down and practically no shifts were observed for R(20). We present these changes in the form of predictive formulas, which would be useful in clinical applications.

摘要

直线加速器治疗头的电子场塑形铈基低熔点合金挡块对输出剂量和百分深度剂量有一定影响。这些由侧向散射不平衡引起的影响在较高能量以及半径较小的挡块中尤为明显。在一个源皮距为100 cm的10×10 cm治疗头中,使用平行板型电离室对圆形、方形和三角形挡块以及开放野进行了剂量测量。绘制了百分深度剂量曲线,并测量了每个挡块的输出剂量。以开放的10×10 cm野为归一化标准,输出因子根据能量、挡块形状和腔面积在0.891至0.996之间变化。使用挡块后,R(100)向表面移动。对于12 MeV和14 MeV,移动范围分别为9至0 mm和13至0 mm,具体取决于形状和腔面积。对于R(90)、R(80)和R(50),观察到的移动范围变窄,而对于R(20),几乎未观察到移动。我们以预测公式的形式呈现这些变化,这在临床应用中会很有用。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a7d7/3249732/b16903af8abc/JMP-36-213-g003.jpg

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