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Beta dose calculation in human arteries for various brachytherapy seed types

机译:各种近距离放射治疗种子类型的人体动脉Beta剂量计算

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摘要

This dissertation explores beta dose profile of microspheres packed in arteries, various source geometries of 142Pr that can be used for therapeutic purpose, and dose backscatter factors for selected beta sources. A novel treatment method by injecting microspheres into feeding arteries of arteriovenous malformation (AVM) is under pre-clinical investigation. To optimize radiation dose to the clinically important area, i.e. arterial wall, preliminary dosimetric studies were needed. Monte Carlo calculations were performed for several geometries simulating arteries filled with microspheres packed by random packing methods. Arterial radii used in the simulation varied from 50 mm to 3 mm; microsphere radii varied from 10 mm to 0.7 mm. Dose varied significantly as a function of microsphere size, for constant arterial sizes. For the same sizes of arteries, significant dose increase was observed because of inter-artery exposure for large arteries (> 0.1 cm rad.) filled with large microspheres (> 0.03 cm rad.). Dose increase between small arteries (0.03 cm rad.) was less significant.The dose profiles of prototype 142Pr beta brachytherapy sources were calculated using MCNP 4C Monte Carlo code as well as dose point kernel (DPK) for selected cases. Dose profiles were similar to beta sources currently used indicating that 142Pr can substitute for current sources for certain cases and the DPK was closely matched with MCNP result.Backscattering of electrons is a prominent secondary effect in beta dosimetry. The backscattering is closely correlated with factors such as geometry of source and scattering material, and composition of scattering material. The backscattering factors were calculated for selected beta sources that are currently used as well as potentially useful sources for therapeutic purpose. The factors were calculated as a function of distance from the interface between water and scatterers. These factors were fit by a simple function for future incorporation into a DPK code. Backscattering effect was significant for short distance from the surface of interface between water and scattering material.
机译:本论文探讨了填充在动脉中的微球的β剂量分布,可用于治疗目的的142Pr的各种源几何形状以及所选β源的剂量反向散射因子。临床前正在研究一种通过将微球体注入动静脉畸形(AVM)的供血动脉中的新型治疗方法。为了优化对临床重要区域即动脉壁的辐射剂量,需要进行初步的剂量学研究。蒙特卡洛(Monte Carlo)计算是针对模拟通过随机填充方法填充的微球填充的动脉的几种几何形状进行的。模拟中使用的动脉半径从50毫米到3毫米不等;微球半径从10毫米到0.7毫米不等。对于恒定的动脉大小,剂量随微球大小而变化很大。对于相同大小的动脉,由于大动脉(> 0.1 cm弧度)充满大微球(> 0.03 cm弧度)的动脉间暴露,观察到剂量明显增加。小动脉之间的剂量增加(弧度为0.03厘米)不太明显。对于所选病例,使用MCNP 4C蒙特卡洛代码以及剂量点核(DPK)计算了原型142Prβ近距离放射治疗源的剂量分布。剂量分布与目前使用的β离子源相似,这表明在某些情况下142Pr可以替代电流源,并且DPK与MCNP结果紧密匹配。电子的反向散射是β剂量法中的主要次要作用。反向散射与诸如源和散射材料的几何形状以及散射材料的组成等因素密切相关。计算了当前使用的选定β源以及用于治疗目的的潜在有用源的反向散射因子。计算这些因子是距离水和散射体之间的距离的函数。这些因素由一个简单的函数拟合,可以将来合并到DPK代码中。对于距水和散射材料之间的界面表面较短的距离,反向散射效果显着。

著录项

  • 作者

    Lee Sung-Woo;

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  • 年度 2004
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  • 原文格式 PDF
  • 正文语种 en_US
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