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首页> 外文期刊>Medical Physics >Radionuclide spatial distribution and dose deposition for in vitro in vitro assessments of 212 212 Pb‐αVCAM‐1 targeted alpha therapy
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Radionuclide spatial distribution and dose deposition for in vitro in vitro assessments of 212 212 Pb‐αVCAM‐1 targeted alpha therapy

机译:放射性核素空间分布和剂量沉积在体外分类,体外评估为212 212 pb-αvcam-1靶向α治疗

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摘要

Purpose Targeted alpha therapy (TAT) takes advantage of the short‐range and high‐linear energy transfer of α‐particles and is increasingly used, especially for the treatment of metastatic lesions. Nevertheless, dosimetry of α‐emitters is challenging for the very same reasons, even for in vitro experiments. Assumptions, such as the uniformity of the distribution of radionuclides in the culture medium, are commonly made, which could have a profound impact on dose calculations. In this study we measured the spatial distribution of α‐emitting 212 Pb coupled to an anti‐VCAM‐1 antibody ( 212 Pb‐αVCAM‐1) and its evolution over time in the context of in vitro irradiations. Methods Two experimental setups were implemented without cells to measure α‐particle count rates and energy spectra in culture medium containing 15?kBq of 212 Pb‐α‐VCAM‐1. Silicon detectors were placed above and below cell culture dishes for 20?h. One of the dishes had a 2.5‐μm‐thick mylar‐base allowing easy detection of the α‐particles. Monte Carlo simulations were performed to analyze experimental spectra. Experimental setups were modeled and α‐energy spectra were simulated in the silicon detectors for different decay positions in the culture medium. Simulated spectra were then used to deconvolute experimental spectra to determine the spatial distribution of 212 Pb‐αVCAM‐1 in the medium. This distribution was finally used to calculate the dose deposition in cell culture experiments. Results Experimental count rates and energy spectra showed differences in measurements taken at the top and the bottom of dishes and temporal variations that did not follow 212 Pb decay. The radionuclide spatial distribution was shown to be composed of a uniform distribution and concentration gradients at the top and the bottom, which were subjected to temporal variations that may be explained by gravity and electrostatic attraction. The absorbed dose in cells calculated from this distribution was compared with the dose expected for a uniform and static distribution and found to be 1.75 times higher, which is highly significant to interpret biological observations. Conclusions This study demonstrated that accurate dosimetry of α‐emitters requires the experimental determination of radionuclide spatial and temporal distribution and highlighted that in vitro assessment of dose for TAT cannot only rely on a uniform distribution of activity in the culture medium. The reliability and reproducibility of future experiments should benefit from specifically developed dosimetry tools and methods.
机译:目的靶向α疗法(TAT)利用α-颗粒的短距和高线性能量转移,越来越多地使用,特别是用于治疗转移性病变。然而,α - 发射剂的剂量法致力于具有相同的原因,即使对于体外实验。通常制备诸如培养基中放射性核素分布的均匀性的假设,这可能对剂量计算产生深远的影响。在该研究中,我们测量了α-发射212pb的空间分布,含有抗VCAM-1抗体(212pb-αvcam-1)及其在体外照射的背景下随时间的演变。方法在没有细胞的情况下实施两种实验设置,以测量含有15μl212pb-α-Vcam-1的培养基中的α-粒子计数率和能谱。将硅探测器置于上方和下方细胞培养皿中20μl。其中一个菜肴具有2.5μm厚的骨髓基础,允许易于检测α-颗粒。进行蒙特卡罗模拟以分析实验光谱。模拟实验装置,在培养基中模拟硅探测器中的α-能谱。然后使用模拟光谱对去核解实验光谱以确定培养基中212pb-αvcam-1的空间分布。该分布最终用于计算细胞培养实验中的剂量沉积。结果实验计率和能谱显示出在顶部和底部的测量和底部的差异,并且不遵循212pb衰减的时间变化。显示放射性核素空间分布显示,顶部和底部的均匀分布和浓度梯度组成,其经受重力和静电吸引的时间变化。将由该分布计算的细胞中的吸收剂量与预期和静态分布的剂量进行比较,发现较高的1.75倍,这对于解释生物观察非常重要。结论本研究表明,α - 发射器的准确剂量测定需要实验测定放射性核素空间和时间分布,并强调的是,对于TAT的剂量的体外评估,不能依赖于培养基中的活性均匀分布。未来实验的可靠性和再现性应受益于专门开发的剂量测定工具和方法。

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