Feasibility of secondary 15O beam production for in-beam PET

A. Mohammadi, Y. Hirano, F. Nishikido, E. Yoshida, A. Kitagawa, T. Inaniwa, T. Yamaya
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引用次数: 2

Abstract

For the purpose of in situ visualization of an irradiation field in particle therapy, it is ideal to use radioactive beams for in-beam positron emission tomography (PET) imaging. In the Heavy Ion Medical Accelerator in Chiba (HIMAC), there is a beam course to produce 11C and 10C as secondary beams, but generation of 15O has never been investigated. This study was devoted to analysis of the feasibility of secondary 15O production for in-beam PET by 16O primary beam in different absorbing materials (targets) with various thicknesses in order to find out the optimum target material and its thickness. The study was performed using analytical method, LISE++ code, and the Monte Carlo method, PHITS code. The calculation results showed that the highest intensity of the secondary 15O beam observed for primary 16O beam decelerating in liquid hydrogen but practically almost impossible to apply. The final optimum target was considered to be polyethylene with thickness of 11 cm. The 15O beam was produced in the HIMAC secondary beam line using the optimum target and the in-beam PET imaging was presented for a PMMA phantom irradiated with the produced beam.
梁内PET二次15O梁生产的可行性
为了在粒子治疗中实现辐照场的原位可视化,使用放射性光束进行束内正电子发射断层扫描(PET)成像是理想的。在千叶重离子医学加速器(HIMAC)中,存在产生11C和10C作为二次光束的光束过程,但从未研究过产生15O的问题。本研究通过分析16O主光束在不同厚度的吸波材料(靶材)中二次生产15O的可行性,找出最佳的靶材及其厚度。研究采用解析法,LISE++代码,蒙特卡罗方法,PHITS代码。计算结果表明,二次15O光束在液氢中减速时强度最高,但实际上几乎不可能应用。最终的最佳目标是厚度为11 cm的聚乙烯。利用最佳目标在HIMAC二次波束线上产生15O波束,并利用所产生的波束辐照PMMA模体进行波束内PET成像。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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