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Dosimetry and clustering properties of energy deposition from beta particles emitted by hydrogen-3 and carbon-14 in the nucleus of a mamalian cell.

机译:哺乳动物细胞核中氢3和碳14发射的β粒子沉积的能量的剂量学和聚类特性。

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It has been suggested that the more densely ionizing terminal portion of an electron track could be responsible for the majority of biological damage as opposed to the less densely ionizing initial part of the track. To test this hypothesis, it is proposed to compare chromosome aberration yields when cell nuclei are irradiated by incorporated 3H and 14 C. The rationale is that virtually all electron tracks from 3H would originate and terminate in the nucleus, whereas almost none of the β particles would stop inside the nucleus for 14C. Since the intention would be to determine RBE values, careful evaluation of dosimetry of β particles from decays of 3H and 14C in the nucleus of a cell is necessary. Three aspects of this dosimetry were addressed: (1) the intranuclear dose, (2) the internuclear dose, and (3) the fraction of dose deposited by electron track ends. A Monte Carlo electron track-structure code was used as the primary tool for solving these problems. Comparisons of results produced by three different Monte Carlo codes in terms of energy deposition in spherical volumes showed good agreement. Track-structure codes were also compared with other analytical methods for beta dosimetry reported in the literature. The intranuclear dose from both radionuclides was calculated for a variety of nuclear sizes under assumptions of spherical and ellipsoidal geometry for a cell nucleus. A method for estimating the internuclear dose for cells with nuclei of different geometries was described. For cells with flat nuclei, similar to those that will be used in the experiments, the internuclear dose was determined to be negligible for 3H and a few percent of the intranuclear dose for 14C. A K-means clustering algorithm was employed to characterize electron track ends. Criteria were developed and implemented in a scoring procedure to identify clusters associated with track ends of primary and secondary electrons and separate these from the less densely ionizing portion of electron tracks. The fraction of dose due to electron track ends was estimated as ∼43% for 3H and ∼30% for 14 C. These values were independent of geometry for a cell nucleus.
机译:已经提出,与电子迹线的初始部分密度较小的相反,电子迹线的更紧密电离的末端部分可能是造成大部分生物损伤的原因。为了验证该假设,建议比较掺入 3 H和 14 C照射细胞核时的染色体畸变产生率。理由是,几乎所有来自 3 H的电子径迹都会在原子核中起始和终止,而对于 14 C,几乎没有β粒子会在原子核内停止。由于意图是确定RBE值,因此有必要仔细评估细胞核中 3 H和 14 C的衰变对β粒子剂量的影响。解决了该剂量测定法的三个方面:(1)核内剂量,(2)核间剂量,(3)电子径迹末端沉积的剂量分数。蒙特卡罗电子轨道结构代码被用作解决这些问题的主要工具。三种不同的蒙特卡洛编码在球形体积中的能量沉积方面产生的结果的比较显示出很好的一致性。轨道结构代码也与文献中报道的用于β剂量测定的其他分析方法进行了比较。在假定细胞核具有球形和椭圆形几何形状的情况下,针对各种核尺寸,从两种放射性核素计算出的核内剂量。描述了一种估计具有不同几何形状细胞核的细胞核间剂量的方法。对于具有扁平核的细胞,类似于将在实验中使用的细胞,对于 3 H,核间剂量被忽略不计,对于 14 ,核内剂量被确定为百分之几。超级> C。采用 K -均值聚类算法表征电子径迹末端。制定了标准并以计分程序实施,以识别与一次和二次电子的轨道末端相关的簇,并将其与电子轨道的密度较小的电离部分分开。对于 3 H,由于电子径迹末端引起的剂量分数估计约为43%,对于 14 C约为30%。这些值与细胞核的几何形状无关。

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