Crosbie J C, Svalbe I, Midgley S M, Yagi N, Rogers P A W, Lewis R A
School of Physics, Monash University, Melbourne, Victoria 3800, Australia.
Phys Med Biol. 2008 Dec 7;53(23):6861-77. doi: 10.1088/0031-9155/53/23/014. Epub 2008 Nov 12.
This paper describes a method of film dosimetry used to measure the peak-to-valley dose ratios for synchrotron microbeam radiation therapy (MRT). Two types of radiochromic film (manufactured by International Specialty Products, NJ, USA) were irradiated in a phantom and also flush against a microbeam collimator (beam width 25 microm, centre-to-centre spacing 200 microm) on beamline BL28 B2 at the SPring-8 synchrotron. Four experiments are reported: (1) the HD-810 and EBT varieties of radiochromic film were used to record 'peak' dose and 'valley' (regions in between peaks) dose, respectively; (2) a stack of HD-810 film sheets was microbeam-irradiated and analysed to investigate a possible dose build-up effect; (3) a very high MRT dose was delivered to HD-810 film to elicit a measurable valley dose to compare with the result obtained using broad beam radiation; (4) the half value layer of the beam with and without the microbeam collimator was measured to investigate the effect of the collimator on the beam quality. The valley dose obtained for films placed flush against the collimator was approximately 0.2% of the peak dose. Within the water phantom, the valley dose had increased to between 0.7 and 1.8% of the peak dose, depending on the depth in the phantom. We also demonstrated, experimentally and by Monte Carlo simulation, that the dose is not maximal on the surface and that there is a dose build-up effect. The microbeam collimator did not make an appreciable difference to the beam quality. The values of the peak-to-valley ratio reported in this paper are higher than those predicted by previously published Monte Carlo simulation papers.
本文描述了一种用于测量同步加速器微束放射治疗(MRT)峰谷剂量比的薄膜剂量测定方法。两种类型的放射变色薄膜(由美国新泽西州国际特殊产品公司制造)在体模中进行了辐照,并且在SPring-8同步加速器的BL28 B2光束线上与微束准直器(束宽25微米,中心间距200微米)紧贴放置。报告了四项实验:(1)分别使用放射变色薄膜的HD-810和EBT品种记录“峰”剂量和“谷”(峰之间的区域)剂量;(2)对一叠HD-810薄膜片进行微束辐照并分析,以研究可能的剂量积累效应;(3)向HD-810薄膜施加非常高的MRT剂量,以得出可测量的谷剂量,以便与使用宽束辐射获得的结果进行比较;(4)测量有和没有微束准直器时光束的半值层,以研究准直器对光束质量的影响。紧贴准直器放置的薄膜获得的谷剂量约为峰剂量的0.2%。在水体模内,谷剂量增加到峰剂量的0.7%至1.8%之间,具体取决于体模中的深度。我们还通过实验和蒙特卡罗模拟证明,剂量在表面并非最大,并且存在剂量积累效应。微束准直器对光束质量没有明显影响。本文报告的峰谷比数值高于先前发表的蒙特卡罗模拟论文所预测的值。