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空心 X 射线微束准直原理用于高对比度细胞质辐照。

Collimation principles of a hollow X-ray microbeam for high-contrast cytoplasm irradiation.

机构信息

Institute of Modern Physics, Fudan University, Shanghai 200433, China.

Key Laboratory of Nuclear Physics and Ion-beam Application (MOE), Fudan University, Shanghai 200433, China.

出版信息

J Radiat Res. 2024 Sep 24;65(5):591-602. doi: 10.1093/jrr/rrae046.

DOI:10.1093/jrr/rrae046
PMID:39154379
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11420837/
Abstract

A Monte Carlo simulation was used to assess the performance of a collimated hollow X-ray microbeam for subcellular cytoplasm irradiation. A high-Z coaxial collimation structure with an inner core for nucleus shielding was investigated. Two key performances, the extraction efficiency (cytoplasm dose per unit incident fluence) and the dose contrast (cytoplasm-to-nucleus dose ratio), were evaluated regarding the influences of the material, geometry and physical arrangements of the collimator, target dish and incident beam source. Simulation results demonstrate that a gold coaxial structure with a practical collimation geometry of a 1-mm length, 10-μm inner diameter and 200-μm outer diameter, with the top exit closely attached (with a minimized air gap) to the bottom of a cell dish with a 3-μm thick Mylar film is recommended for cytoplasm irradiation of adherent mammalian cells. For a synchrotron source in the energy range < 10 keV, a dose contrast of approximately 100 can be achieved. For a bremsstrahlung source <30-kV tube voltage, a dose contrast of approximately 50-100 can still be achieved. General principles are summarized with further explanations of the performance of the hollow X-ray microbeam.

摘要

采用蒙特卡罗模拟方法评估了用于亚细胞细胞质辐照的准直中空 X 射线微束的性能。研究了一种带有用于屏蔽核的内芯的高 Z 同轴准直结构。针对准直器、靶盘和入射束源的材料、几何形状和物理布置的影响,评估了两个关键性能,即提取效率(单位入射通量的细胞质剂量)和剂量对比度(细胞质与细胞核的剂量比)。模拟结果表明,对于贴壁哺乳动物细胞的细胞质辐照,推荐使用具有实际准直几何形状(长度为 1 毫米、内径为 10 微米、外径为 200 微米)的金同轴结构,其顶部出口与具有 3 微米厚聚酯薄膜的细胞盘的底部紧密贴合(最小化空气间隙)。对于能量范围 <10 keV 的同步加速器源,可以实现约 100 的剂量对比度。对于 <30 kV 管电压的韧致辐射源,仍可以实现约 50-100 的剂量对比度。总结了一般原则,并进一步解释了中空 X 射线微束的性能。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4dd7/11420837/00951755d07d/rrae046f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4dd7/11420837/189e16ebfda8/rrae046f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4dd7/11420837/f6fc79fa1abf/rrae046f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4dd7/11420837/f86cff5dd3a4/rrae046f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4dd7/11420837/fdbeab39c96d/rrae046f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4dd7/11420837/9af1fcdd19ad/rrae046f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4dd7/11420837/c78de33c4bf2/rrae046f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4dd7/11420837/8655f02d4c58/rrae046f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4dd7/11420837/00951755d07d/rrae046f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4dd7/11420837/189e16ebfda8/rrae046f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4dd7/11420837/f6fc79fa1abf/rrae046f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4dd7/11420837/f86cff5dd3a4/rrae046f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4dd7/11420837/fdbeab39c96d/rrae046f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4dd7/11420837/9af1fcdd19ad/rrae046f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4dd7/11420837/c78de33c4bf2/rrae046f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4dd7/11420837/8655f02d4c58/rrae046f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4dd7/11420837/00951755d07d/rrae046f8.jpg

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