Sato Tatsuhiko, Manabe Kentaro, Hamada Nobuyuki
Research Group for Radiation Protection, Japan Atomic Energy Agency (JAEA), Shirakata Shirane 2-4, Tokai, Ibaraki, Japan.
Radiation Safety Research Center, Nuclear Technology Research Laboratory, Central Research Institute of Electric Power Industry (CRIEPI), 2-11-1 Iwado-kita, Komae, Tokyo, Japan.
PLoS One. 2014 Jun 11;9(6):e99831. doi: 10.1371/journal.pone.0099831. eCollection 2014.
The risk of internal exposure to 137Cs, 134Cs, and 131I is of great public concern after the accident at the Fukushima-Daiichi nuclear power plant. The relative biological effectiveness (RBE, defined herein as effectiveness of internal exposure relative to the external exposure to γ-rays) is occasionally believed to be much greater than unity due to insufficient discussions on the difference of their microdosimetric profiles. We therefore performed a Monte Carlo particle transport simulation in ideally aligned cell systems to calculate the probability densities of absorbed doses in subcellular and intranuclear scales for internal exposures to electrons emitted from 137Cs, 134Cs, and 131I, as well as the external exposure to 662 keV photons. The RBE due to the inhomogeneous radioactive isotope (RI) distribution in subcellular structures and the high ionization density around the particle trajectories was then derived from the calculated microdosimetric probability density. The RBE for the bystander effect was also estimated from the probability density, considering its non-linear dose response. The RBE due to the high ionization density and that for the bystander effect were very close to 1, because the microdosimetric probability densities were nearly identical between the internal exposures and the external exposure from the 662 keV photons. On the other hand, the RBE due to the RI inhomogeneity largely depended on the intranuclear RI concentration and cell size, but their maximum possible RBE was only 1.04 even under conservative assumptions. Thus, it can be concluded from the microdosimetric viewpoint that the risk from internal exposures to 137Cs, 134Cs, and 131I should be nearly equivalent to that of external exposure to γ-rays at the same absorbed dose level, as suggested in the current recommendations of the International Commission on Radiological Protection.
福岛第一核电站事故后,公众高度关注体内暴露于137Cs、134Cs和131I的风险。由于对它们微剂量分布差异的讨论不足,相对生物效应(本文定义为体内暴露相对于γ射线外照射的效应)有时被认为远大于1。因此,我们在理想排列的细胞系统中进行了蒙特卡罗粒子输运模拟,以计算137Cs、134Cs和131I发射的电子体内暴露以及662 keV光子外照射在亚细胞和核内尺度上吸收剂量的概率密度。然后根据计算出的微剂量概率密度,推导由于亚细胞结构中放射性同位素(RI)分布不均匀以及粒子轨迹周围高电离密度导致的相对生物效应。考虑到旁观者效应的非线性剂量响应,也从概率密度估计了其相对生物效应。由于高电离密度导致的相对生物效应和旁观者效应的相对生物效应非常接近1,因为体内暴露和662 keV光子外照射的微剂量概率密度几乎相同。另一方面,由于RI不均匀性导致的相对生物效应在很大程度上取决于核内RI浓度和细胞大小,但即使在保守假设下,它们的最大可能相对生物效应也仅为1.04。因此,从微剂量学观点可以得出结论,正如国际放射防护委员会目前的建议中所指出的,在相同吸收剂量水平下,体内暴露于137Cs、134Cs和131I的风险应与γ射线外照射的风险几乎相当。