University of Pennsylvania, Perelman School of Medicine, Department of Radiation Oncology, Philadelphia, United States of America.
Phys Med Biol. 2023 Jul 10;68(14). doi: 10.1088/1361-6560/ace14d.
. A physicochemical model built on the radiochemical kinetic theory was recently proposed in (Labarbe2020) to explain the FLASH effect. We performed extensive simulations to scrutinize its applicability for oxygen depletion studies and FLASH-related experiments involving both proton and electron beams.. Using the dose and beam delivery parameters for each FLASH experiment, we numerically solved the radiochemical rate equations comprised of a set of coupled nonlinear ordinary differential equations to obtain the area under the curve (AUC) of radical concentrations.. The modeled differences in AUC induced by ultra-high dose rates appeared to correlate well with the FLASH effect. (i) For the whole brain irradiation of mice performed in (Montay-Gruel2017), the threshold dose rate values for memory preservation coincided with those at which AUC started to decrease much less rapidly. (ii) For the proton pencil beam scanning FLASH of (Cunningham2021), we found linear correlations between radicals' AUC and the biological endpoints: TGF-1, leg contracture and plasma level of cytokine IL-6. (iii) Compatible with the findings of the proton FLASH experiment in (Kim2021), we found that radicals' AUC at the entrance and mid-Spread-Out Bragg peak regions were highly similar. In addition, our model also predicted ratios of oxygen depletion-values between normal and UHDR irradiation similar to those observed in (Cao2021) and (El Khatib2022).. Collectively, our results suggest that the normal tissue sparing conferred by UHDR irradiation may be due to the lower degree of exposure to peroxyl and superoxide radicals. We also found that the differential effect of dose rate on the radicals' AUC was less pronounced at lower initial oxygen levels, a trait that appears to align with the FLASH differential effect on normal versus tumor tissues.
. 最近,(Labarbe2020)提出了一个基于放射性化学动力学理论的物理化学模型,以解释FLASH 效应。我们进行了广泛的模拟,以仔细研究其在氧耗竭研究和涉及质子和电子束的 FLASH 相关实验中的适用性。. 使用每个 FLASH 实验的剂量和束流输送参数,我们通过数值求解由一组耦合非线性常微分方程组成的放射性化学速率方程,得到自由基浓度的曲线下面积(AUC)。. 超高剂量率引起的 AUC 差异与 FLASH 效应似乎密切相关。(i)在(Montay-Gruel2017)进行的小鼠全脑照射实验中,记忆保存的阈值剂量率值与 AUC 开始显著下降的剂量率值一致。(ii)对于(Cunningham2021)的质子铅笔束扫描 FLASH,我们发现自由基 AUC 与生物终点之间存在线性相关性:TGF-1、腿部挛缩和细胞因子 IL-6 的血浆水平。(iii)与质子 FLASH 实验的发现一致(Kim2021),我们发现入口和展宽布拉格峰区的自由基 AUC 高度相似。此外,我们的模型还预测了正常和 UHDR 照射之间的氧耗值比值与(Cao2021)和(El Khatib2022)观察到的相似。. 总之,我们的结果表明,超高剂量率照射赋予正常组织的保护作用可能是由于暴露于过氧自由基和超氧自由基的程度较低。我们还发现,在初始氧水平较低时,剂量率对 AUC 的影响差异较小,这一特征似乎与 FLASH 对正常组织与肿瘤组织的差异效应一致。