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首页> 外文期刊>Health Physics: Official Journal of the Health Physics Society >SECONDARY NEUTRON DOSES TO PEDIATRIC PATIENTS DURING INTRACRANIAL PROTON THERAPY: MONTE CARLO SIMULATION OF THE NEUTRON ENERGY SPECTRUM AND ITS ORGAN DOSES
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SECONDARY NEUTRON DOSES TO PEDIATRIC PATIENTS DURING INTRACRANIAL PROTON THERAPY: MONTE CARLO SIMULATION OF THE NEUTRON ENERGY SPECTRUM AND ITS ORGAN DOSES

机译:中子中子剂量在颅内质子治疗期间给小儿患者:中子能量谱的蒙特卡罗模拟及其器官剂量

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Proton therapy has the physical advantage of a Bragg peak that can provide a better dose distribution than conventional x-ray therapy. However, radiation exposure of normal tissues cannot be ignored because it is likely to increase the risk of secondary cancer. Evaluating secondary neutrons generated by the interaction of the proton beam with the treatment beam-line structure is necessary; thus, performing the optimization of radiation protection in proton therapy is required. In this research, the organ dose and energy spectrum were calculated from secondary neutrons using Monte Carlo simulations. The Monte Carlo code known as the Particle and Heavy Ion Transport code System (PHITS) was used to simulate the transport proton and its interaction with the treatment beam-line structure that modeled the double scattering body of the treatment nozzle at the National Cancer Center Hospital East. The doses of the organs in a hybrid computational phantom simulating a 5-y-old boy were calculated. In general, secondary neutron doses were found to decrease with increasing distance to the treatment field. Secondary neutron energy spectra were characterized by incident neutrons with three energy peaks: 1x10(-7), 1, and 100 MeV. A block collimator and a patient collimator contributed significantly to organ doses. In particular, the secondary neutrons from the patient collimator were 30 times higher than those from the first scatter. These results suggested that proactive protection will be required in the design of the treatment beam-line structures and that organ doses from secondary neutrons may be able to be reduced.
机译:质子疗法具有比常规X射线治疗的更好剂量分布的布拉格峰的物理优势。然而,正常组织的辐射暴露不能被忽略,因为它可能会增加继发性癌症的风险。评估通过质子梁与处理梁线结构的相互作用产生的二级中子是必要的;因此,需要在质子疗法中进行优化辐射保护。在该研究中,使用Monte Carlo模拟从二级中子计算器官剂量和能谱。称为粒子和重离子传输代码系统(PHITS)的蒙特卡罗代码用于模拟运输质子及其与处理梁线结构的相互作用,该结构在国家癌症中心医院建模治疗喷嘴的双散射体东。计算了混合计算幻影中的器官的剂量,模拟了一个5-Y老男孩的模拟。通常,发现次要中子剂量随着与处理领域的增加而降低。二级中子能谱的特征在于入射中子,具有三个能量峰:1×10(-7),1和100meV。块准直器和患者准直器对器官剂量有显着贡献。特别地,来自患者准直器的二级中子比来自第一散射的二级中子高30倍。这些结果表明,在处理梁线结构的设计中,将需要主动保护,并且可以减少来自二级中子的器官剂量。

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