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Dose distributions in phantoms with different dimensions exposed to BNCT epithermal neutron beam: measurements and calculations

机译:用不同尺寸暴露于BNCT骨骺梁的不同尺寸的模子:测量和计算

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Boron neutron capture therapy (BNCT) is a cancer treatment still in development that is considered with increasing interest It consists in irradiating with thermal or epithermal neutrons patients to whom a specific tumor-seeking Boron carrier has been administrated. The high cross section of the ~(10)B(n,α)~7Li reaction for thermal neutrons and the high radiobiological effectiveness are exploited in order to damage the tumour cells without afflicting the surrounding healthy tissues. Nowadays, adequate neutron fluxes for BNCT treatments can be provided by nuclear reactors. For each neutron source, it is important to measure the dose distribution in tissue equivalent phantoms in order to characterize the radiation field and to acquire useful data exploited by the treatment planning system to calculate the dose distribution in the patient. In the epithermal column of the LVR-1S reactor at NRI Rez (CZ) a series of measurements were performed with FriXy-gel dosimeters inserted in a standard parallelepiped (40 × 40 × 20 cm~3) water phantom and in a cylindrical (d = 16cm, h = 14cm) water-equivalent phantom. FriXy gels are based on ferrous sulphate solution (Fricke solution) containing Xylenol-Orange infused in a porcine skin 3 mm-thick matrix. The dosimeters are imaged with a CCD camera system before and after irradiation, and the measured difference of optical density at 585 nm wavelength is proportional to the absorbed dose. In particular, boron dose distributions have been evaluated using 16 × 14 × 0.3 cm~3 dosimeters placed along the beam axis. In the two phantoms, similar boron capture distributions have been found on the beam axis; on the opposite hand, more relevant differences have been detected off-axis, showing a not negligible difference of distribution of the thermal neutron flux in the standard phantom and in a volume with head dimensions. In-depth measurements and off-axis profiles were compared with Monte Carlo simulations performed with MCNP5, showing good consistency.
机译:硼中子捕获疗法(BNCT)是仍在开发中的癌症治疗,随着越来越多的兴趣,它包括辐射热量或膜中子患者,患有特定的寻求巨型硼载体的患者。用于热中子的〜(10)B(n,α)〜7li反应的高横截面和高辐射生物学效应,以损害肿瘤细胞而不粘在周围的健康组织。如今,可以通过核反应堆提供足够的BNCT处理中子丝量。对于每个中子源,重要的是测量组织当量模拟中的剂量分布,以表征辐射场并获取由治疗计划系统利用的有用数据来计算患者的剂量分布。在NRI REZ(CZ)的LVR-1S反应器的曲线柱中,通过插入标准平行六面体(40×40×20cm〜3)水体模谱和圆柱形(D.)的Frixy-Gel剂量计进行一系列测量。 = 16cm,h = 14厘米)水当量的幽灵。 Frixy凝胶基于含有硫酸硫代硫酸氢溶液(FRICKE溶液),其含有猪皮3mm厚的基质中的含有木烯醇 - 橙。在照射之前和之后,用CCD相机系统对剂量计进行成像,并且在585nm波长下测量的光密度差异与吸收剂量成比例。特别地,已经使用沿梁轴放置的16×14×0.3cm〜3剂量计进行了评估了硼剂量分布。在两个幻影中,在梁轴上发现了类似的硼捕获分布;在相反的手上,偏离轴上检测到更相关的差异,显示标准模型中的热中子通量的分布不可忽略的差异,并且具有带头尺寸的体积。与MCNP5进行的蒙特卡罗模拟进行比较深入测量和轴外轮廓,显示出良好的一致性。

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