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Estimation of the response function of a PADC based neutron dosimeter in terms of fluence and H_p(10)

机译:基于能量密度和H_p(10)的基于PADC的中子剂量计的响应函数估计

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The UAB PADC-based neutron dosimeter consists of a 500 μm thick Poly Allyl Diglicol Carbonate layer, covered with polyethylene, to originate protons from fast neutrons through elastic (n,p) scattering, with Makrofol, to flatten the energy response of the dosimeter, especially at high neutron energies, and with Nylon, where protons of 626 keV are produced through the ~(14)N(n,p)~(14)C reaction from incident thermal neutrons. Extensive work was performed in the past to characterise the Hp(10) response of this neutron dosimeter, with exposures to reference monoenergetic fields as well as to ISO radionuclide based sources. In the present work, all known information about the dosimeter response R is gathered in order to build the response curves as a function of incident neutron energy in terms of fluence, RΦ(E), and in terms of personal dose equivalent, R Hp(10)(E), for normally incident neutrons. Once RΦ(E) is known, the calculated dosimeter readings when exposed to known neutron fields (SIGMA source (IRSN, Cadarache) and several ISO sources) are evaluated and compared to experimental measurements. Calculated and experimental values agree within uncertainties for the SIGMA source and the ~(241)Am-Be and ~(252)Cf sources, while differences about 20% appear for the D_2O moderated sources, which have an important contribution of intermediate energy neutrons. An average value of 350 cm~(-2) mSv~(-1) for the coefficient K relating dosimeter reading with personal dose equivalent allows determining neutron personal equivalent doses in the range ~200 keV-12 MeV with an overall standard uncertainty below 50%, as required for routine operational neutron personal dosimetry.
机译:基于UAB PADC的中子剂量计由一个500μm厚的聚乙二酸乙二醇酯碳酸酯层组成,覆盖有聚乙烯,通过Makrofol通过弹性(n,p)散射从快中子产生质子,从而使剂量计的能量响应平坦,特别是在高中子能的情况下,在尼龙中,入射热中子通过〜(14)N(n,p)〜(14)C反应生成626 keV质子。过去进行了大量工作来表征该中子剂量计的Hp(10)响应,并暴露于参考单能场以及基于ISO放射性核素的辐射源。在当前工作中,收集了有关剂量计响应R的所有已知信息,以便根据通量RΦ(E)和个人剂量当量R Hp(R)建立响应曲线作为入射中子能量的函数。 10)(E),用于正常入射的中子。一旦知道RΦ(E),就将暴露于已知中子场(SIGMA源(IRSN,Cadarache)和几个ISO源)的计算的剂量计读数进行评估,并与实验测量值进行比较。对于SIGMA源以及〜(241)Am-Be和〜(252)Cf源,计算值和实验值在不确定性范围内一致,而D_2O调节源的差异约为20%,这对中间能量中子起重要作用。与剂量计读数和个人剂量当量相关的系数K的平均值为350 cm〜(-2)mSv〜(-1),可以确定〜200 keV-12 MeV范围内的中子个人当量剂量,总体标准不确定度低于50 %,按常规操作中子个人剂量法的要求。

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