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首页> 外文期刊>Physics in medicine and biology. >A new approach to the determination of air kerma using primary-standard cavity ionization chambers.
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A new approach to the determination of air kerma using primary-standard cavity ionization chambers.

机译:一种使用初级标准腔室电离室确定空气比释动能的新方法。

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摘要

A consistent formalism is presented using Monte Carlo calculations to determine the reference air kerma from the measured energy deposition in a primary-standard cavity ionization chamber. A global approach avoiding the use of cavity ionization theory is discussed and its limitations shown in relation to the use of the recommended value for W. The role of charged-particle equilibrium is outlined and the consequent requirements placed on the calculations are detailed. Values for correction factors are presented for the BIPM air-kerma standard for 60Co, making use of the Monte Carlo code PENELOPE, a detailed geometrical model of the BIPM 60Co source and event-by-event electron transport. While the wall correction factor k(wall) = 1.0012(2) is somewhat lower than the existing value, the axial non-uniformity correction k(an) = 1.0027(3) is significantly higher. The use of a point source in the evaluation of k(an) is discussed. A comparison is made of the calculated dose ratio with the Bragg-Gray and Spencer-Attix stopping-power ratios, the results indicating a preference for the Bragg-Gray approach in this particular case. A change to the recommended value for W of up to 2 parts in 10(3) is discussed. The uncertainties arising from the geometrical models, the use of phase-space files, the radiation transport algorithms and the underlying radiation interaction coefficients are estimated.
机译:使用蒙特卡洛计算法来确定一致的形式,以根据在标准腔内电离室中测得的能量沉积来确定参考空气比释动能。讨论了避免使用腔电离理论的全局方法,并显示了与使用W推荐值有关的局限性。概述了带电粒子平衡的作用,并详细说明了对计算的要求。通过使用蒙特卡罗代码PENELOPE,BIPM 60Co源的详细几何模型和逐事件电子传输,为60Co的BIPM空气比释动能标准提供了校正因子的值。尽管壁校正因子k(wall)= 1.0012(2)略低于现有值,但轴向不均匀校正k(an)= 1.0027(3)明显更高。讨论了在k(an)评估中使用点源。将计算出的剂量比与Bragg-Gray和Spencer-Attix停止功率比进行比较,结果表明在这种特殊情况下偏爱Bragg-Gray方法。讨论了在10(3)中最多将W的推荐值更改为2的部分。估计了由几何模型,相空间文件的使用,辐射传输算法和潜在的辐射相互作用系数引起的不确定性。

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