首页> 外文期刊>Physics in medicine and biology. >A Monte Carlo study of absorbed dose distributions in both the vapor and liquid phases of water by intermediate energy electrons based on different condensed-history transport schemes.
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A Monte Carlo study of absorbed dose distributions in both the vapor and liquid phases of water by intermediate energy electrons based on different condensed-history transport schemes.

机译:蒙特卡洛研究基于不同的凝结历史传输方案的中间能电子对水在气相和液相中吸收剂量分布的研究。

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摘要

Monte Carlo transport calculations of dose point kernels (DPKs) and depth dose profiles (DDPs) in both the vapor and liquid phases of water are presented for electrons with initial energy between 10 keV and 1 MeV. The results are obtained by the MC4 code using three different implementations of the condensed-history technique for inelastic collisions, namely the continuous slowing down approximation, the mixed-simulation with delta-ray transport and the addition of straggling distributions for soft collisions derived from accurate relativistic Born cross sections. In all schemes, elastic collisions are simulated individually based on single-scattering cross sections. Electron transport below 10 keV is performed in an event-by-event mode. Differences on inelastic interactions between the vapor and liquid phase are treated explicitly using our recently developed dielectric response function which is supplemented by relativistic corrections and the transverse contribution. On the whole, the interaction coefficients used agree to better than approximately 5% with NIST/ICRU values. It is shown that condensed phase effects in both DPKs and DDPs practically vanish above 100 keV. The effect of delta-rays, although decreases with energy, is sizeable leading to more diffused distributions, especially for DPKs. The addition of straggling for soft collisions is practically inconsequential above a few hundred keV. An extensive benchmarking with other condensed-history codes is provided.
机译:对于初始能量在10 keV和1 MeV之间的电子,给出了水的汽相和液相中剂量点内核(DPK)和深度剂量分布图(DDP)的蒙特卡洛输运计算。结果是通过MC4代码使用非历史碰撞的压缩历史技术的三种不同实现方式获得的,即连续减慢逼近度,带有增量射线传输的混合模拟以及为精确碰撞而获得的软碰撞散布分布相对论天生的横截面。在所有方案中,弹性碰撞都是基于单散射截面单独模拟的。在逐事件模式下执行低于10 keV的电子传输。气相和液相之间非弹性相互作用的差异已使用我们最近开发的介电响应函数进行了明确处理,该函数通过相对论校正和横向贡献得到了补充。总体而言,所使用的相互作用系数与NIST / ICRU值相比约好5%。结果表明,在100 keV以上,DPK和DDP中的凝结相位效应实际上消失了。 δ射线的影响虽然随能量而减小,但相当大,导致分布更加分散,尤其是对于DPK。在几百keV以上,为软碰撞而增加的杂散实际上是无关紧要的。提供了与其他压缩历史代码的广泛基准测试。

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