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Monte Carlo simulations of neutron spectral fluence, radiation weighting factor and ambient dose equivalent for a passively scattered proton therapy unit

机译:被动散射质子治疗装置的中子光谱注量,辐射加权因子和等效环境剂量的蒙特卡罗模拟

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Stray neutron exposures pose a potential risk for the development of secondary cancer in patients receiving proton therapy. However, the behavior of the ambient dose equivalent is not fully understood, including dependences on neutron spectral fluence, radiation weighting factor and proton treatment beam characteristics. The objective of this work, therefore, was to estimate neutron exposures resulting from the use of a passively scattered proton treatment unit. In particular, we studied the characteristics of the neutron spectral fluence, radiation weighting factor and ambient dose equivalent with Monte Carlo simulations. The neutron spectral fluence contained two pronounced peaks, one a low-energy peak with a mode around 1 MeV and one a high-energy peak that ranged from about 10 MeV up to the proton energy. The mean radiation weighting factors varied only slightly, from 8.8 to 10.3, with proton energy and location for a closed-aperture configuration. For unmodulated proton beams stopped in a closed aperture, the ambient dose equivalent from neutrons per therapeutic absorbed dose (H*(10)/D) calculated free-in-air ranged from about 0.3 mSv/Gy for a small scattered field of 100 MeV proton energy to 19 mSv/Gy for a large scattered field of 250 MeV proton energy, revealing strong dependences on proton energy and field size. Comparisons of in-air calculations with in-phantom calculations indicated that the in-air method yielded a conservative estimation of stray neutron radiation exposure for a prostate cancer patient.
机译:接受质子治疗的患者中流离失所的中子暴露可能会继发癌症。但是,还没有完全了解环境剂量当量的行为,包括对中子光谱注量,辐射权重因子和质子处理束特性的依赖性。因此,这项工作的目的是评估由于使用被动分散的质子处理单元而导致的中子暴露。特别是,我们使用蒙特卡洛模拟研究了中子谱注量,辐射加权因子和等效环境剂量的特性。中子光谱注量包含两个明显的峰,一个是低能峰,其模态约为1 MeV,另一个是高能峰,其范围从约10 MeV到质子能量。平均辐射权重因子仅在8.8到10.3之间变化,其质子能量和位置为闭孔配置。对于停在封闭孔径中的未调制质子束,对于100 MeV的小散射场,在空中计算的中子每治疗吸收剂量的等效环境剂量(H *(10)/ D)约为0.3 mSv / Gy。对于250 MeV质子能量的大散射场,质子能达到19 mSv / Gy,这显示出对质子能量和场大小的强烈依赖性。空中计算与幻像计算的比较表明,空中方法对前列腺癌患者产生了杂散中子辐射暴露的保守估计。

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