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首页> 外文期刊>Physics in medicine and biology. >Dose distribution of secondary radiation in a water phantom for a proton pencil beam-EURADOS WG9 intercomparison exercise
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Dose distribution of secondary radiation in a water phantom for a proton pencil beam-EURADOS WG9 intercomparison exercise

机译:质子铅笔射线辐射水幻影中辐射的二次辐射剂量分布

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摘要

Systematic 3D mapping of out-of-field doses induced by a therapeutic proton pencil scanning beam in a 300 x 300 x 600 mm(3) water phantom was performed using a set of thermoluminescence detectors (TLDs): MTS-7 ((LiF)-Li-7:Mg, Ti), MTS-6 ((LiF)-Li-6:Mg, Ti), MTS-N ((LiF)-Li-nat:Mg, Ti) and TLD-700 ((LiF)-Li-7: Mg, Ti), radiophotoluminescent (RPL) detectors GD-352M and GD-302M, and polyallyldiglycol carbonate (PADC)-based (C12H18O7) track-etched detectors. Neutron and gamma-ray doses, as well as linear energy transfer distributions, were experimentally determined at 200 points within the phantom. In parallel, the Geant4 Monte Carlo code was applied to calculate neutron and gamma radiation spectra at the position of each detector. For the cubic proton target volume of 100 x 100 x 100 mm(3) (spread out Bragg peak with a modulation of 100 mm) the scattered photon doses along the main axis of the phantom perpendicular to the primary beam were approximately 0.5 mGy Gy(-1) at a distance of 100 mm and 0.02 mGy Gy(-1) at 300 mm from the center of the target. For the neutrons, the corresponding values of dose equivalent were found to be similar to 0.7 and similar to 0.06 mSv Gy(-1), respectively. The measured neutron doses were comparable with the out-offield neutron doses from a similar experiment with 20 MV x-rays, whereas photon doses for the scanning proton beam were up to three orders of magnitude lower.
机译:使用一组热致发光探测器(TLD)进行300×300×600mm(3)水体模具,通过一组热辐发光探测器(PTS-7((LIF),进行系统3D映射由治疗性质子铅笔扫描梁诱导的野外铅笔扫描梁诱导的外场剂量。((LIF) -li-7:mg,ti),mts-6((Lif)-li-6:mg,ti),mts-n((Lif)-li-nat:mg,ti)和tld-700((Lif )-LI-7:Mg,Ti),放射透射发光(RPL)检测器GD-352M和GD-302M,以及基于聚烯烃(C12H18O7)轨道蚀刻探测器的聚烯烃碳酸盐(PADC)。中子和γ射线剂量,以及线性能量转移分布在体模内的200点处实验确定。并行地,施加了Geant4蒙特卡罗代码以计算每个检测器位置的中子和伽马辐射光谱。对于100×100×100mm(3)的立方质子靶体积(用调节展开100 mm的布拉格峰),沿着主梁的虚线主轴散射的光子剂量约为0.5 mgy gy( -1)距离目标中心为100毫米和0.02 mgy(-1)的距离,距离距离的300毫米。对于中子,发现剂量等同物的相应值类似于0.7和类似于0.06msv Gy(-1)。测量的中子剂量与来自20mV X射线类似的实验的外放大中子剂量相当,而扫描质子束的光子剂量达到较低的三个数量级。

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