首页> 外文期刊>Nuclear Technology >SIMULATION OF THE CHARGE PRODUCED BY PROTONS INSIDE A TISSUE EQUIVALENT IONIZATION CHAMBER IN A MIXED NEUTRON/GAMMA FIELD IN BNCT
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SIMULATION OF THE CHARGE PRODUCED BY PROTONS INSIDE A TISSUE EQUIVALENT IONIZATION CHAMBER IN A MIXED NEUTRON/GAMMA FIELD IN BNCT

机译:BNCT中子/伽马混合场中质子当量电离室内质子产生的电荷的模拟

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摘要

The neutron and gamma dose in boron neutron capture therapy (BNCT) can be determined by using ioniza-tion chambers of different materials. However, inexplicable results, such as negative doses, are sometimes obtained. Computer simulations using MCNPX can help one to understand the behavior of ionization chambers. This paper deals with a part of this investigation: the contribution of protons to the total measured charge in a tissue equivalent (TE) ionization chamber that is flushed with methane-based TE gas. The inherent problem is that the Monte Carlo code MCNPX cannot track protons below 1 MeV.rnA custom-made program, called Proton Produced Ionization Chamber Charge (PPICC), calculates the deposited energy and thus the charge in the TE gas per proton. For this, it uses the stopping powers for protons in TE plastic and gas. MCNPX provides the total number of protons produced by all neutron interactions near the gas. To checkrnthis new procedure, measurements and simulations have been performed using a validated mixed beam of neutrons and gammas. The neutronfluence consists of 12 % fast neutrons and 87% epithermal neutrons. In one setup the chamber is free-in-air (epithermal/fast neutron field) and in the other is in a cubic polymethylmethacrylate phantom at 25 mm depth (thermal/epithermal neutron field).rnThe total charge is the sum of the charges due to electrons, originating from primary and neutron-induced gammas, and protons from ~1H(n,n) ~1H and ~(14)N(n,p)~(14)C reactions. The total measured and calculated charges in the two setups have acceptable uncertainties and are in good agreement. The charge collected in a TE ionization chamber can be simulated in a mixed field of neutrons and gammas. The charge resulting from proton recoil in the gas is unexpectedly large.
机译:硼中子俘获疗法(BNCT)中的中子和伽马剂量可以通过使用不同材料的电离室来确定。但是,有时会得到莫名其妙的结果,例如负剂量。使用MCNPX进行计算机模拟可以帮助人们了解电离室的行为。本文涉及这一研究的一部分:质子对在被甲烷基TE气体冲洗的组织当量(TE)电离室中总测得电荷的贡献。固有的问题是蒙特卡罗代码MCNPX无法跟踪低于1 MeV的质子。一个名为“质子产生的电离室电荷”(PPICC)的定制程序可以计算沉积的能量,从而计算每个质子在TE气体中的电荷。为此,它使用TE塑料和气体中的质子作为制动力。 MCNPX提供了气体附近所有中子相互作用产生的质子总数。为了检验这一新程序,已经使用经过验证的中子和伽马混合束进行了测量和模拟。中子通量由12%的快中子和87%的超热中子组成。在一种设置中,腔室是自由空气的(中子/快中子场),在另一种腔中是25mm深度的立方聚甲基丙烯酸甲酯幻影(热/中子场).rn总电荷是应得电荷的总和。到电子,这些电子来自于初级和中子诱发的伽玛射线,以及来自〜1H(n,n)〜1H和〜(14)N(n,p)〜(14)C反应的质子。两种设置中测得的总费用和计算出的费用具有可接受的不确定性,并且吻合良好。可以在中子和伽马混合场中模拟TE电离室中收集的电荷。气体中质子反冲产生的电荷异常大。

著录项

  • 来源
    《Nuclear Technology》 |2009年第1期|29-34|共5页
  • 作者单位

    Joint Research Centre, Institute for Energy, P.O. Box 2, Petten, 1755 ZG, The Netherlands University of Bucharest, Faculty of Physics, P.O. Box MG-1, 76900, Romania;

    National Tsing Hua University, Department of Engineering and System Science, Hsinchu 30013, Taiwan;

    Joint Research Centre, Institute for Energy, P.O. Box 2, Petten, 1755 ZG, The Netherlands;

    NCT Physics, Nassaulaan 12, Alkmaar, 1815 GK, The Netherlands;

    Joint Research Centre, Institute for Energy, P.O. Box 2, Petten, 1755 ZG, The Netherlands;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    MCNPX; ionization chamber; mixed field;

    机译:MCNPX;电离室混合场;
  • 入库时间 2022-08-18 00:44:14

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