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在聚焦放疗计划系统中实施增强动态楔形板。

Implementation of enhanced dynamic wedge in the focus rtp system.

作者信息

Miften M, Wiesmeyer M, Beavis A, Takahashi K, Broad S

机构信息

Computerized Medical Systems, Inc., St. Louis. MO 63132, USA.

出版信息

Med Dosim. 2000 Summer;25(2):81-6. doi: 10.1016/s0958-3947(00)00033-9.

Abstract

The FOCUS RTP system implementation of Varian's enhanced dynamic wedge (EDW) is presented. Calculations of both dose distributions and wedge factors (WFs) are based on segmented treatment tables (STTs). Calculating dose requires a "transmission matrix" derived from an STT to model the modified fluence from the source. The dose calculation is then performed using either the Clarkson or convolution/superposition algorithms. An initial "primary dose/monitor unit (MU) fraction" WF estimate at the weight point of symmetric and asymmetric fields is calculated from the STT as the ratio of MU delivered on the axis of the weight point divided by total MU delivered for the treatment field. In our approach, we go beyond this initial estimate with a "scatter dose" correction. This requires measured 60 degrees WFs for 5 fields. Scatter corrections derived from measured WFs are interpolated for other wedge angles and field sizes in much the same way as arbitrary wedge angle STTs are derived from a "golden STT" using the "ratio of tangents" formalism. Dose comparisons with measured distributions show good agreement to within 3% or 3 mm for 6-MV beams and all EDW angles. Agreement with measurements to within 1% is obtained for WFs in all symmetric and asymmetric fields for 6- and 10-MV beams. For large wedge angles and field sizes, this represents a significant improvement over the 3% to 4% errors often observed using the MU fraction model alone.

摘要

介绍了瓦里安增强型动态楔形板(EDW)的FOCUS RTP系统实现。剂量分布和楔形因子(WFs)的计算均基于分段治疗表(STTs)。计算剂量需要从STT导出的“传输矩阵”来模拟源的修正注量。然后使用克拉克森算法或卷积/叠加算法进行剂量计算。对称和不对称射野权重点处的初始“主剂量/监测单位(MU)分数”WF估计值是根据STT计算得出的,即权重点轴上输送的MU与治疗射野输送的总MU之比。在我们的方法中,我们通过“散射剂量”校正对这一初始估计值进行改进。这需要测量5个射野的60度WFs。从测量的WFs得出的散射校正值可通过与从“黄金STT”使用“正切比”形式导出任意楔形角STT大致相同的方式,内插到其他楔形角和射野尺寸。与测量分布的剂量比较显示,对于6兆伏(MV)射线束和所有EDW角度,在3%或3毫米范围内具有良好的一致性。对于6兆伏和10兆伏射线束的所有对称和不对称射野中的WFs,与测量值的一致性在1%以内。对于大楔形角和射野尺寸,这比仅使用MU分数模型时经常观察到的3%至4%的误差有显著改善。

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