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Decomposition of the dose conversion factor based on fluence spectra of secondary charged particles: Application to lateral dose profiles in photon fields

机译:基于二次带电粒子的流量光谱的剂量转化系数分解:光子田中横向剂量分析

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Purpose The dose conversion factor plays an important role in the dosimetry by enabling the absorbed dose in the sensitive volume of a detector to be converted into the absorbed dose in the surrounding medium (in most cases water). The purpose of this paper is to demonstrate that a specific fluence‐based approach for the decomposition of the dose conversion factor is in particular useful for the interpretation of the influences of detector properties on measurements under nonreference conditions. Methods Data for the dose conversion factor and secondary fluence spectra were obtained by the Monte Carlo method. The calculation of the secondary charged particle fluence (electrons and positrons) in the sensitive detector volume was imbedded into the code for the calculation of absorbed dose in the detector. The decomposition method into subfactors is based on the use of these fluence data applied to a stepwise transition from the dose at the point of measurement next to a pure water detector and finally to the fully simulated detector geometry. Each subfactor is obtained as a ratio, at which the stopping power only is different in the numerator and the denominator or at which the fluence only is different in the numerator and the denominator. This method was applied at photon dose profiles obtained in water at different radiation qualities and with various detectors of cylindrical type. Results The resulting subfactors can be well identified as a stopping power ratio and as perturbation factors each reflecting particular detector properties. Two of them ( f 1 and f 4 ) are equivalent with perturbation factors which have already been introduced by other authors previously. These are the volume perturbation factor and the extracameral perturbation factor. Subfactor f 2 denoted as medium perturbation factor was found to resemble the density perturbation factor. Results obtained for the volume perturbation factor applied to dose profiles measured with cylindrical detectors confirm that the volume effect can be well described by a convolution of the true profile in water with a Gaussian kernel. It was found that the sigma parameter depends on the cylinder radius only and amounts almost exactly to half of its value. The medium perturbation factor strongly depends on the density of the detector medium. For an air‐filled detector, the influence of the air again can be described by a Gauss convolution, however, with a less good agreement. For detectors with a density of the cavity medium larger than that of water, for instance, for a diamond detector, it was found that there is a tendency of compensation between the volume averaging effect and the medium effect. Conclusion The fluence‐based decomposition of the dose conversion factor leads to a fluence‐based formulation of perturbation factors, referred to as volume, medium, and extracameral perturbation factor. These factors offer useful explanations for the behavior of detectors in nonreference conditions. An example was given for cylindrical detectors at dose profile measurements.
机译:目的的剂量转换因子起着通过使得能够在检测器的敏感体积中的吸收剂量中的剂量测定了重要的作用被转换为在周围介质中的吸收剂量(在大多数情况下的水)。本文的目的是证明,对于剂量转换因子分解的基于注量的具体做法是特别是用于检测器性能的影响的非引用上的条件下的测量的解释是有用的。方法数据用于剂量转换因子和次级通量光谱通过蒙特卡罗方法获得。在敏感检测器体积中的次生带电粒子通量(电子和正电子)的计算被嵌入到用于吸收剂量的在检测器的计算的代码。分解法成子因素是基于使用在测量点旁边的一个纯净水检测器,最后到完全模拟检测器的几何形状从剂量施加到逐步过渡这些注量数据。每个子因素是作为比率,在该停止功率仅是在分子和分母或在其中注量仅是在分子和分母不同不同而获得。此方法在光子应用的剂量在不同的辐射特性在水中获得的简档和与圆柱型的各种检测器。结果所得到的子因子可以很好地识别为停止功率比和作为扰动因素每个反射特定检测器的性能。它们中的两个(f 1和f 4)是等价的与已引入由其他作者先前扰动因素。这些都是体积扰动因子和扰动extracameral因素。子因素F 2表示为介质扰动因素被发现类似于密度扰动因素。该卷扰动因素中获得的结果应用到剂量与圆柱形探测器确认音量效果可以很好通过实际轮廓的卷积在水中与高斯核描述测量配置文件。结果发现,西格玛参数仅取决于圆柱半径和金额几乎完全以它的价值的一半。该介质扰动因素强烈地依赖于检测器介质的密度。对于一个充满空气的检测,空气的影响又可以通过高斯卷积描述,然而,有一个不太好的协议。用于与所述腔介质比水大的密度检测器,例如,对于检测器的金刚石,人们发现,有体积平均效应和介质之间效应补偿的倾向。结论剂量转换因子导致的扰动因素中,被称为体积,中和extracameral扰动因子基于注量的制剂的基于注量分解。这些因素提供探测器在非引用条件的行为非常有用的解释。一个例子给出在剂量分布的测量圆筒探测器。

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