Division of Biomedical Engineering, University of Saskatchewan, Saskatoon, Canada.
Phys Med Biol. 2020 Apr 3;65(7):075010. doi: 10.1088/1361-6560/ab7361.
Microbeam radiation therapy (MRT) utilizes highly collimated synchrotron generated x-rays to create narrow planes of high dose radiation for the treatment of tumors. Individual microbeams have a typical width of 30-50 µm and are separated by a distance of 200-500 µm. The dose delivered at the center of the beam is lethal to cells in the microbeam path, on the order of hundreds of Grays (Gy). The tissue between each microbeam is spared and helps aid in the repair of adjacent damaged tissue. Radiation interactions within the peak of the microbeam, such as the photoelectric effect and incoherent (atomic Compton) scattering, cause some dose to be delivered to the valley areas adjacent to the microbeams. As the incident x-ray energy is modified, radiation interactions within a material change and affect the probability of interactions, as well as the directionality and energy of ionizing particles (electrons) that deposit energy in the valley regions surrounding the microbeam peaks. It is crucial that the valley dose between microbeams be minimal to maintain the effectiveness of MRT. Using a monochromatic x-ray source with x-ray energies ranging from 30 to 150 keV, a detailed investigation into the effect of incident x-ray energy on the dose profiles of microbeams was performed using samarium doped fluoroaluminate (FA) glass as the medium. All dosimetric measurements were carried out using a purpose-built fluorescence confocal microscope dosimetric technique that used Sm-doped FA glass plates as the irradiated medium. Dose profiles are measured over a very a wide range of x-ray energies at micrometer resolution and dose distribution in the microbeam are mapped. The measured microbeam profiles at different energies are compared with the MCNP6 radiation transport code, a general transport code which can calculate the energy deposition of electrons as they pass through a given material. The experimentally measured distributions can be used to validate the results for electron energy deposition in fluoroaluminate glass. Code validation is necessary for using transport codes in future treatment planning for MRT and other radiation therapies. It is shown that simulated and measured micro beam-profiles are in good agreement, and micrometer level changes can be observed using this high-resolution dosimetry technique. Full width at 10% of the maximum peak (FW@10%) was used to quantify the microbeam width. Experimental measurements on FA glasses and simulations on the dependence of the FW@10% at various energies are in good agreement. Simulations on energy deposited in water indicate that FW@10% reaches a local minimum around energies 140 keV. In addition, variable slit width experiments were carried out at an incident x-ray energy of 100 keV in order to determine the effect of the narrowing slit width on the delivered peak dose. The microbeam width affects the peak dose, which decreases with the width of the microbeam. Experiments suggest that a typical microbeam width for MRT is likely to be between 20-50 µm based on this work.
微束放射治疗(MRT)利用高度准直的同步加速器产生的 X 射线,为肿瘤治疗创建高剂量辐射的狭窄平面。单个微束的典型宽度为 30-50μm,间隔距离为 200-500μm。光束中心的剂量对微束路径中的细胞是致命的,数量级为数百格雷(Gy)。每个微束之间的组织不受影响,有助于辅助相邻受损组织的修复。微束内的辐射相互作用,如光电效应和非相干(原子康普顿)散射,导致一些剂量传递到微束相邻的谷区。随着入射 X 射线能量的改变,材料内的辐射相互作用发生变化,并影响相互作用的概率,以及在微束峰周围的谷区沉积能量的电离粒子(电子)的方向性和能量。至关重要的是,微束之间的谷剂量要最小化,以保持 MRT 的有效性。使用能量范围为 30 至 150keV 的单色 X 射线源,使用掺钐氟铝酸盐(FA)玻璃作为介质,对入射 X 射线能量对微束剂量分布的影响进行了详细研究。所有剂量测量均使用专门设计的荧光共焦显微镜剂量测量技术进行,该技术使用掺钐 FA 玻璃片作为辐照介质。在非常宽的 X 射线能量范围内以微米分辨率测量剂量分布,并绘制微束中的剂量分布。在不同能量下测量的微束轮廓与 MCNP6 辐射输运代码进行比较,MCNP6 是一种通用输运代码,可以计算电子在穿过给定材料时的能量沉积。实验测量的分布可用于验证氟铝酸盐玻璃中电子能量沉积的结果。在未来的 MRT 和其他放射治疗计划中使用输运代码,必须进行代码验证。结果表明,模拟和测量的微束轮廓吻合良好,使用这种高分辨率剂量测量技术可以观察到微米级的变化。全宽的 10%(FW@10%)用于量化微束宽度。FA 玻璃的实验测量和各种能量下 FW@10%的模拟结果吻合良好。水的能量沉积模拟表明,FW@10%在约 140keV 的能量下达到局部最小值。此外,在入射 X 射线能量为 100keV 时进行了可变狭缝宽度实验,以确定狭缝变窄对传递峰值剂量的影响。微束宽度会影响峰值剂量,随着微束宽度的减小而减小。实验表明,基于这项工作,MRT 的典型微束宽度可能在 20-50μm 之间。