Mojżeszek N, Farah J, Kłodowska M, Ploc O, Stolarczyk L, Waligórski M P R, Olko P
Institute of Nuclear Physics, Polish Academy of Sciences (IFJ PAN), Radzikowskiego 152, 31-342 Krakow, Poland.
Institut de Radioprotection et de Sûreté Nucléaire (IRSN), Pôle Radioprotection de l'Homme, BP-17, 92260 Fontenay-aux-Roses, France; Hôpitaux Universitaires Paris-Sud, Pôle Imagerie et Médecine Nucléaire, Hôpital du Kremlin-Bicêtre, 78 Rue Général Leclerc, 94270 Le Kremlin-Bicêtre, France(1).
Phys Med. 2017 Feb;34:80-84. doi: 10.1016/j.ejmp.2017.01.013. Epub 2017 Jan 25.
To measure the environmental doses from stray neutrons in the vicinity of a solid slab phantom as a function of beam energy, field size and modulation width, using the proton pencil beam scanning (PBS) technique.
Measurements were carried out using two extended range WENDI-II rem-counters and three tissue equivalent proportional counters. Detectors were suitably placed at different distances around the RW3 slab phantom. Beam irradiation parameters were varied to cover the clinical ranges of proton beam energies (100-220MeV), field sizes ((2×2)-(20×20)cm) and modulation widths (0-15cm).
For pristine proton peak irradiations, large variations of neutron H(10)/D were observed with changes in beam energy and field size, while these were less dependent on modulation widths. H(10)/D for pristine proton pencil beams varied between 0.04μSvGy at beam energy 100MeV and a (2×2)cm field at 2.25m distance and 90° angle with respect to the beam axis, and 72.3μSvGy at beam energy 200MeV and a (20×20) cm field at 1m distance along the beam axis.
The obtained results will be useful in benchmarking Monte Carlo calculations of proton radiotherapy in PBS mode and in estimating the exposure to stray radiation of the patient. Such estimates may be facilitated by the obtained best-fitted simple analytical formulae relating the stray neutron doses at points of interest with beam irradiation parameters.
使用质子笔形束扫描(PBS)技术,测量固体平板模体附近杂散中子产生的环境剂量,作为束流能量、射野大小和调制宽度的函数。
使用两个扩展量程的WENDI-IIrem计数器和三个组织等效正比计数器进行测量。探测器适当地放置在RW3平板模体周围的不同距离处。改变束流照射参数,以覆盖质子束能量(100 - 220MeV)、射野大小((2×2)-(20×20)cm)和调制宽度(0 - 15cm)的临床范围。
对于原始质子峰照射,随着束流能量和射野大小的变化,观察到中子H(10)/D有很大变化,而这些变化对调制宽度的依赖性较小。原始质子笔形束的H(10)/D在束流能量100MeV、射野(2×2)cm、距离2.25m且相对于束轴成90°角时为0.04μSv/Gy,在束流能量200MeV、射野(20×20)cm、沿束轴距离1m时为72.3μSv/Gy。
所得结果将有助于对PBS模式下质子放疗的蒙特卡罗计算进行基准测试,并有助于估计患者受到的杂散辐射剂量。通过获得的将感兴趣点的杂散中子剂量与束流照射参数相关联的最佳拟合简单解析公式,可能会促进此类估计。