Department of Accelerator and Medical Physics, National Institute of Radiological Sciences, QST, Chiba, Japan.
Department of Basic Medical Sciences for Radiation Damages, National Institute of Radiological Sciences, QST, Chiba, Japan.
Int J Radiat Oncol Biol Phys. 2020 Mar 1;106(3):597-603. doi: 10.1016/j.ijrobp.2019.10.040. Epub 2019 Oct 31.
The purpose is to verify experimentally whether application of magnetic fields longitudinal and perpendicular to a proton beam alters the biological effectiveness of the radiation.
Proton beams with linear energy transfer of 1.1 and 3.3 keV/μm irradiated human cancer and normal cells under a longitudinal (perpendicular) magnetic field of B (B) = 0, 0.3, or 0.6 T. Cell survival curves were constructed to evaluate the effects of the magnetic fields on the biological effectiveness. The ratio of dose that would result in a survival fraction of 10% without the magnetic field D to the dose with the magnetic field D, R = D/D, was determined for each cell line and magnetic field.
For cancer cells exposed to the 1.1- (3.3-) keV/μm proton beams, Rs were increased to 1.10 ± 0.07 (1.11 ± 0.07) and 1.11 ± 0.07 (1.12 ± 0.07) by the longitudinal magnetic fields of B = 0.3 and 0.6 T, respectively. For normal cells, Rs were increased to 1.13 ± 0.06 (1.17 ± 0.06) and 1.17 ± 0.06 (1.30 ± 0.06) by the Bs. In contrast, Rs were not changed significantly from 1 by the perpendicular magnetic fields of B = 0.3 and 0.6 T for both cancer and normal cells exposed to 1.1- and 3.3-keV/μm proton beams.
The biological effectiveness of proton beams was significantly enhanced by longitudinal magnetic fields of B = 0.3 and 0.6 T, whereas the biological effectiveness was not altered by perpendicular magnetic fields of the same strengths. This enhancement effect should be taken into account in magnetic resonance imaging guided proton therapy with a longitudinal magnetic field.
验证磁场沿质子束纵向和横向施加是否会改变辐射的生物效应。
线性能量转移为 1.1 和 3.3 keV/μm 的质子束在纵向(横向)磁场 B(B)= 0、0.3 或 0.6 T 下辐照人癌细胞和正常细胞。构建细胞存活曲线以评估磁场对生物效应的影响。对于没有磁场的情况下导致存活分数为 10%的剂量 D 和有磁场的情况下的剂量 D,确定每个细胞系和磁场的比值 R = D/D。
对于暴露于 1.1-(3.3-)keV/μm 质子束的癌细胞,纵向磁场 B = 0.3 和 0.6 T 分别将 Rs 增加到 1.10 ± 0.07(1.11 ± 0.07)和 1.11 ± 0.07(1.12 ± 0.07)。对于正常细胞,纵向磁场 B = 0.3 和 0.6 T 将 Rs 分别增加到 1.13 ± 0.06(1.17 ± 0.06)和 1.17 ± 0.06(1.30 ± 0.06)。相比之下,暴露于 1.1-和 3.3-keV/μm 质子束的癌细胞和正常细胞的横向磁场 B = 0.3 和 0.6 T 对 Rs 没有显著影响,仍为 1。
纵向磁场 B = 0.3 和 0.6 T 显著增强了质子束的生物效应,而相同强度的横向磁场则没有改变生物效应。在具有纵向磁场的磁共振成像引导质子治疗中,应考虑这种增强效应。