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Monte Carlo modelling of diode detectors for small field MV photon dosimetry: Detector model simplification and the sensitivity of correction factors to source parameterization

机译:用于小场MV光子剂量测定的二极管探测器的蒙特卡洛建模:探测器模型简化以及校正因子对源参数化的敏感性

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The goal of thisworkwas to examine the use of simplified diode detector models within a recently proposed Monte Carlo (MC) based small field dosimetry formalism and to investigate the influence of electron source parameterization has on MC calculated correction factors. BEAMnrc was used to model Varian 6 MV jaw-collimated square field sizes down to 0.5 cm. The IBA stereotactic field diode (SFD), PTW T60016 (shielded) and PTW T60017 (un-shielded) diodes were modelled in DOSRZnrc and isocentric output ratios (OR fclin detMC) calculated at depths of d = 1.5, 5.0 and 10.0 cm. Simplified detector models were then tested by evaluating the percent difference in OR fclin detMC between the simplified and complete detector models. The influence of active volume dimension on simulated output ratio and response factor was also investigated. The sensitivity of each MC calculated replacement correction factor (k fclin, fmsr Qclin,Qmsr), as a function of electron FWHM between 0.100 and 0.150 cm and energy between 5.5 and 6.5 MeV, was investigated for the same set of small field sizes using the simplified detector models. The SFD diode can be approximated simply as a silicon chip in water, the T60016 shielded diode can be modelled as a chip in water plus the entire shielding geometry and the T60017 unshielded diode as a chip in water plus the filter plate located upstream. The detectorspecific k fclin, fmsr Qclin,Qmsr required to correct measured output ratios using the SFD, T60016 and T60017 diode detectors are insensitive to incident electron energy between 5.5 and 6.5MeV and spot size variation between FWHM = 0.100 and 0.150 cm. Three general conclusions come out of thiswork: (1) detector models can be simplified to produce OR fclin detMC to within 1.0% of those calculated using the complete geometry, where typically not only the silicon chip, but also any high density components close to the chip, such as scattering plates or shielding material is necessary to be included in the model, (2) diode detectors of smaller active radius require less of a correction and (3) k fclin, fmsr Qclin,Qmsr is insensitive to the incident the electron energy and spot size variations investigated. Therefore, simplified detector models can be used with acceptable accuracy within the recently proposed small field dosimetry formalism.
机译:这项工作的目的是在最近提出的基于蒙特卡洛(MC)的小场剂量学形式学中研究简化二极管检测器模型的使用,并研究电子源参数化对MC计算的校正因子的影响。 BEAMnrc用于建模Varian 6 MV颚式准直的方形场,尺寸小至0.5 cm。以DOSRZnrc和等密度输出比(OR fclin detMC)对IBA立体定向场二极管(SFD),PTW T60016(带屏蔽)和PTW T60017(非屏蔽)二极管进行建模,并在d = 1.5、5.0和10.0 cm的深度处进行计算。然后,通过评估简化探测器模型和完整探测器模型之间的OR fclin detMC差异百分比来测试简化的探测器模型。还研究了有效容积尺寸对模拟输出比和响应因子的影响。对于同一组小场尺寸,研究了每个MC计算的替换校正因子(k fclin,fmsr Qclin,Qmsr)的灵敏度,该灵敏度是电子FWHM在0.100至0.150 cm之间以及能量在5.5至6.5 MeV之间的函数。简化的探测器模型。 SFD二极管可以简单地近似为水中的硅芯片,T60016屏蔽二极管可以模拟为水中的芯片加上整个屏蔽几何形状,T60017非屏蔽二极管可以模拟为水中的芯片加上上游的滤板。使用SFD,T60016和T60017二极管检波器校正测量输出比所需的特定于检测器的k fclin,fmsr Qclin,Qmsr对5.5至6.5MeV的入射电子能量以及FWHM = 0.100至0.150 cm的光斑尺寸变化不敏感。这项工作得出了三个一般性结论:(1)可以简化检测器模型,以将ORfclin detMC生成为使用完整几何计算得出的ORfclin detMC的1.0%以内,其中通常不仅是硅芯片,而且还有任何接近芯片的高密度组件该模型中必须包含诸如散射板或屏蔽材料之类的芯片,(2)主动半径较小的二极管检测器需要较少的校正,并且(3)k fclin,fmsr Qclin,Qmsr对电子的入射不敏感研究了能量和光斑尺寸的变化。因此,简化的探测器模型可以在最近提出的小场剂量学形式学中以可接受的精度使用。

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