Namur Research Institute For Life Science (NARILIS), Research center for the Physics of Matter and Radiation (PMR-LARN), University of Namur, B-5000, Namur, Belgium.
Biomedical Magnetic Resonance Group (REMA), Louvain Drug Research Institute, Université Catholique de Louvain, B-1200, Woluwé Saint Lambert, Belgium.
Med Phys. 2017 Aug;44(8):4299-4312. doi: 10.1002/mp.12362. Epub 2017 Jul 4.
PURPOSE: To identify which physical properties of nanoparticles are correlated with the survival fraction of cells exposed in vitro to low-energy protons in combination with nanoparticles. METHODS: The Geant4 simulation toolkit (version 10.3) was used to model nanoparticles of different sizes (5-50 nm) and materials (Ti, Zr, Hf, Ta, Au, Pt), with or without an organic capping ensuring biocompatibility and to irradiate them with 1.3 or 4 MeV protons and 5.3 MeV alpha particles. The spectra of secondary electrons inside and at the nanoparticle surface were computed, as well as electron yields, Auger and organic capping contribution, trapping in metal bulk and linear energy transfer profiles as a function of distance from the nanoparticle center. In a next step, an in silico cell model was designed and loaded with gold nanoparticles, according to experimental uptake values. Dose to the cell was evaluated macroscopically and microscopically in 100 × 100 × 100 nm³ voxels for different radiation qualities. RESULTS: The cell geometry showed that radiation enhancement is negligible for the gold concentration used and for any radiation quality. However, when the single nanoparticle geometry is considered, we observed a local LET in its vicinity considerably higher than for the water equivalent case (up to 5 keV/μm at the titanium nanoparticle surface compared to 2.5 keV/μm in the water case). The yield of secondary electrons per primary interaction with 1.3 MeV protons was found to be most favorable for titanium (1.54), platinum (1.44), and gold (1.32), although results for higher Z metals are probably underestimated due to the incomplete simulation of de-excitation cascade in outer shells. It was also found that the organic capping contributed mostly to the production of low-energy electrons, adding a spike of dose near the nanoparticle surface. Indeed, the yield for the coated gold nanoparticle increased to 1.53 when exposed to 1.3 MeV protons. Although most electrons are retained inside larger nanoparticles (50 nm), it was shown that their yield is comparable to smaller sizes and that the linear energy transfer profile is better. From a combination of ballistic and nanoparticle size factors, it was concluded that 10-nm gold nanoparticles were better inducers of additional cell killing than 5-nm gold nanoparticles, matching our previous in vitro study. CONCLUSIONS: Although effects from a physical standpoint are limited, the high linear energy transfer profile at the nanoparticle surface generates detrimental events in the cell, in particular ROS-induced damage and local heating.
目的:确定纳米颗粒的哪些物理特性与体外低能质子与纳米颗粒共同照射下细胞的存活分数相关。
方法:使用 Geant4 模拟工具包(版本 10.3)对不同尺寸(5-50nm)和材料(Ti、Zr、Hf、Ta、Au、Pt)的纳米颗粒进行建模,这些纳米颗粒具有或没有确保生物相容性的有机外壳,并使用 1.3 或 4MeV 质子和 5.3MeV 阿尔法粒子对其进行辐照。计算了纳米颗粒内部和表面的二次电子谱,以及电子产额、俄歇和有机外壳贡献、金属体中的捕获和线性能量转移分布随纳米颗粒中心距离的函数。在下一步中,根据实验摄取值,设计了一个包含金纳米颗粒的虚拟细胞模型。用不同的辐射质量在 100×100×100nm³体素中宏观和微观地评估细胞剂量。
结果:细胞几何形状表明,对于所使用的金浓度和任何辐射质量,辐射增强都可以忽略不计。然而,当考虑单个纳米颗粒的几何形状时,我们观察到其附近的局部 LET 明显高于水当量情况(钛纳米颗粒表面高达 5keV/μm,而水情况为 2.5keV/μm)。发现 1.3MeV 质子与初级相互作用的二次电子产额对钛(1.54)、铂(1.44)和金(1.32)最有利,尽管由于外壳退激发级联的不完全模拟,较高 Z 金属的结果可能被低估。还发现有机外壳主要有助于产生低能电子,在纳米颗粒表面附近增加了剂量尖峰。事实上,当用 1.3MeV 质子照射时,涂覆金纳米颗粒的产额增加到 1.53。尽管大多数电子被保留在较大的纳米颗粒(50nm)中,但结果表明它们的产额与较小尺寸相当,并且线性能量转移分布更好。从弹道和纳米颗粒尺寸因素的组合中得出结论,10nm 金纳米颗粒比 5nm 金纳米颗粒更能诱导额外的细胞杀伤,这与我们之前的体外研究结果相匹配。
结论:尽管从物理角度来看,影响有限,但纳米颗粒表面的高线性能量转移剖面会在细胞中产生有害事件,特别是 ROS 诱导的损伤和局部加热。
Phys Med Biol. 2014-3-21
Phys Med Biol. 2012-5-9
Int J Part Ther. 2024-8-8
Mater Horiz. 2023-10-2
Cancers (Basel). 2020-7-23
Nanomaterials (Basel). 2019-2-19