Poignant Floriane, Monini Caterina, Testa Étienne, Beuve Michaël
Univ. Lyon, Univ. Claude Bernard Lyon 1, CNRS/IN2P3, IP2I Lyon, F-69622, Villeurbanne, France.
Med Phys. 2021 Apr;48(4):1874-1883. doi: 10.1002/mp.14576. Epub 2021 Mar 11.
For the past two decades, high-Z nanoparticles have been of high interest to improve the therapeutic outcomes of radiation therapy, especially for low-energy x-rays. Monte Carlo (MC) simulations have been used to evaluate the boost of dose deposition induced by Auger electrons near the nanoparticle surface, by calculating average energy deposition at the nanoscale. In this study, we propose to go beyond average quantities and quantify the stochastic nature of energy deposition at such a scale. We present results of probability density of the specific energy (restricted to ionization, excitation and electron attachment events) in cylindrical nanotargets of height and radius set at 10 nm. This quantity was evaluated for nanotargets located within 200 nm around 5-50 nm gold nanoparticles (GNPs), for 20-90 keV photon irradiation.
This nanodosimetry study was based on the MC simulation MDM that allows tracking of electrons down to thermalization energy. We introduced a new quantity, namely the probability enhancement ratio (PER), by estimating the probability of imparting to nanotargets a restricted specific energy larger than a threshold (1, 10, and 20 kGy), normalized to the probability for pure water. The PER was calculated as a function of the distance between the nanotarget and the GNP surface. The threshold values were chosen in light of the biophysical model NanOx that predicts cell survival by calculating local lethal events based on the restricted specific energy and an effective local lethal function. then represents a threshold above which the nanotarget damages induce efficiently cell death.
Our calculations showed that the PER varied a lot with the GNP radius, the photon energy, and the distance of the GNP to the nanotarget. The highest PER was 95 when the nanotarget was located at 5 nm from the GNP surface, for a photon energy of 20 keV, a threshold of 20 kGy, and a GNP radius of 50 nm. This enhancement dramatically decreased with increasing GNP-nanotarget distances as it went below 1.5 for distances larger than 200 nm.
The PER seems better adapted than the mean dose deposition to describe the formation of biological damages. The significant increase of the PER within 200 nm around the GNP suggests that severe damages could occur for biological nanotargets located near the GNP. These calculations will be used as an input of the biophysical model NanOx to convert PER into estimation of radiation-induced cell death enhanced by GNPs.
在过去二十年中,高原子序数纳米粒子对于改善放射治疗的疗效备受关注,尤其是对于低能X射线。蒙特卡罗(MC)模拟已被用于通过计算纳米尺度上的平均能量沉积来评估纳米粒子表面附近俄歇电子引起的剂量沉积增强。在本研究中,我们提议超越平均量,量化这种尺度下能量沉积的随机性质。我们给出了高度和半径均设定为10纳米的圆柱形纳米靶中特定能量(限于电离、激发和电子附着事件)的概率密度结果。该量针对位于5至50纳米金纳米粒子(GNP)周围200纳米内的纳米靶进行了评估,用于20至90千电子伏光子照射。
这项纳米剂量学研究基于MC模拟MDM,它能够追踪电子直至热化能量。我们通过估计赋予纳米靶大于阈值(1、10和20千戈瑞)的受限特定能量的概率,并将其归一化为纯水的概率,引入了一个新的量,即概率增强比(PER)。PER作为纳米靶与GNP表面之间距离的函数进行计算。阈值是根据生物物理模型NanOx选择的,该模型通过基于受限特定能量和有效局部致死函数计算局部致死事件来预测细胞存活。那么就代表了一个阈值,高于该阈值纳米靶损伤会有效诱导细胞死亡。
我们的计算表明,PER随GNP半径、光子能量以及GNP与纳米靶的距离有很大变化。当纳米靶位于距GNP表面5纳米处,光子能量为20千电子伏,阈值为20千戈瑞,GNP半径为50纳米时,最高PER为95。随着GNP - 纳米靶距离增加,这种增强显著降低,当距离大于200纳米时降至1.5以下。
PER似乎比平均剂量沉积更适合描述生物损伤的形成。GNP周围200纳米内PER的显著增加表明位于GNP附近的生物纳米靶可能会发生严重损伤。这些计算将用作生物物理模型NanOx的输入,以将PER转换为对GNP增强的辐射诱导细胞死亡的估计。