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Range verification of radioactive ion beams of C-11 and O-15 using in-beam PET imaging

机译:使用束梁宠物成像的C-11和O-15的放射性离子束的范围验证

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In advanced ion therapy, the visualization of the range of incident ions in a patient's body is important for exploiting the advantages of this type of therapy. It is ideal to use radioactive ion beams for in-beam positron emission tomography (PET) imaging in particle therapy due to the high quality of PET images caused by the high signal-to-noise ratio. We have shown the feasibility of this idea through an in-beam PET study for C-11 and O-15 ion beams using the dedicated OpenPET system. In this work, we investigate the potential difference between the Bragg peak position and the position of the maximum detected positron-emitting fragments by a PET system for the radioactive beams of C-11 and O-15. For this purpose, we measured the depth dose in a water phantom and performed PET scans of an irradiated PMMA phantom for the available beams of C-11 and O-15 at the Heavy Ion Medical Accelerator in Chiba (HIMAC). Then, we simulated the depth dose profiles in the water phantom and the yield of the positron-emitting fragments in a PMMA phantom for both available beams using the Monte Carlo code PHITS. The positions of the Bragg peak and maximum positron-emitting fragments from the measurements were well reproduced by simulation. The effect of beam energy broadening on the positional differences between two peaks was studied by simulating an irradiated PMMA phantom. The differences in position between the Bragg peak and the maximum positron-emitting fragments increased when the beam energy spread was broadened, although the differences were zero for the ideal mono-energetic beams. Greater differences were observed for C-11 ion beams compared to O-15 ion beams, although both beams had the same range in water, and the higher energy corresponded to a larger difference. For the known energy spread of the beams, the predicted differences between two peaks from the simulation were consistent with the measured data within submillimetre agreement.
机译:在先进的离子疗法中,患者体内的入射离子范围的可视化对于利用这种类型的疗法的优点是重要的。由于由高信噪比引起的高质量的PET图像,它是使用用于束中束正电子发射断层扫描(PET)成像的放射性离子束的理想选择。我们通过使用专用的开普特系统的C-11和O-15离子束的束和O-15离子梁的束缚宠物研究表明了这个想法的可行性。在这项工作中,我们研究了BRAGG峰位置与最大检测到的正电子发射片段的潜在差,通过PET系统用于C-11和O-15的放射性束。为此目的,我们测量水体模具中的深度剂量,并在千叶(HIMAC)的重离子医疗加速器中的C-11和O-15的可用光束进行辐照的PMMA幻影的PET扫描。然后,我们模拟水体模拟的深度剂量曲线以及使用Monte Carlo Code Phits的PMMA幻像中的PMMA幻像中的正电子发射片段的产量。通过模拟,Bragg峰值和来自测量的最大正电子发射片段的位置很好地再现。通过模拟照射的PMMA幻影研究了光束能量扩展对两个峰之间的位置差的影响。虽然理想的单能级梁为零,但是当光束能量扩展扩大时,布拉格峰与最大正电子发射片段之间的位置的差异增加。对于与O-15离子束相比,对于C-11离子束观察到更大的差异,尽管两个光束在水中具有相同的范围,并且较高的能量对应于更大的差异。对于梁的已知能量扩展,从模拟中的两个峰之间的预测差异与亚瑟尔赛协议中的测量数据一致。

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