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基于蒙特卡罗的适用于兆伏级光子射束不均匀体模中电离室剂量学的校正因子。

Monte Carlo-based correction factors for ion chamber dosimetry in heterogeneous phantoms for megavoltage photon beams.

机构信息

Department of Health Sciences, Kumamoto University, Kumamoto, Japan.

出版信息

Phys Med Biol. 2012 Nov 21;57(22):7615-27. doi: 10.1088/0031-9155/57/22/7615. Epub 2012 Oct 26.

Abstract

The purpose of this study was to investigate the perturbation correction factors and inhomogeneity correction factors (ICFs) for a thin-walled cylindrical ion chamber in a heterogeneous phantom including solid water, lung and bone plastic materials. The perturbation factors due to the replacement of the air cavity, non-water equivalence of the wall and the stem, non-air equivalence of the central electrode and the overall perturbation factor, P(Q), for a cylindrical chamber, in the heterogeneous phantom were calculated with the EGSnrc/Cavity Monte Carlo code for 6 and 15 MV photon beams. The PTW31010 (0.125 cm(3)) chamber was modeled with Monte Carlo simulations, and was used for measurements and calculations of percentage depth ionization (PDI) or percentage depth dose (PDD). ICFs were calculated from the ratio of the product of the stopping power ratios (SPRs) and P(Q) of lung or bone to solid water. Finally, the measured PDIs were converted to PDDs by using ICFs and were compared with those calculated by the Monte Carlo method. The perturbation effect for the ion chamber in lung material is insignificant at 5 × 5 and 10 × 10 cm(2) fields, but the effect needs to be considered under conditions of lateral electron disequilibrium with a 3 × 3 cm(2) field. ICFs in lung varied up to 2% and 4% depending on the field size for 6 and 15 MV, respectively. For bone material, the perturbation effects due to the chamber wall and the stem were more significant at up to 3.5% and 1.6% for 6 MV, respectively. ICFs for bone material were approximately 0.945 and 0.940 for 6 and 15 MV, respectively. The converted PDDs by using ICFs were in good agreement with Monte Carlo calculated PDDs. The chamber perturbation correction and SPRs should strictly be considered for ion chamber dosimetry in heterogeneous media. This is more important for small field dosimetry in lung and bone materials.

摘要

本研究旨在探讨薄壁圆柱电离室在包含固体水、肺和骨塑料材料的不均匀体模中的扰动量校正因子和不均匀性校正因子(ICF)。使用 EGSnrc/Cavity 蒙特卡罗代码计算了 6 和 15 MV 光子束在不均匀体模中,由于空气腔的替代、壁和杆的非水等效性、中央电极的非空气等效性以及圆柱室的整体扰动量校正因子 P(Q)。使用蒙特卡罗模拟对 PTW31010(0.125 cm3)室进行建模,并用于测量和计算百分深度电离(PDI)或百分深度剂量(PDD)。ICF 是通过肺或骨的比阻止本领(SPR)与固体水的乘积与 P(Q)的比值计算得到的。最后,通过使用 ICF 将测量的 PDI 转换为 PDD,并与蒙特卡罗方法计算的 PDD 进行比较。在 5×5 和 10×10 cm2 射野下,电离室在肺材料中的扰动量可以忽略不计,但在 3×3 cm2 射野下存在侧向电子失衡时需要考虑该效应。6 和 15 MV 时,ICF 分别在肺中根据射野大小变化最大为 2%和 4%。对于骨材料,由于壁和杆的影响,6 MV 时分别最大达到 3.5%和 1.6%。6 和 15 MV 时骨材料的 ICF 分别约为 0.945 和 0.940。使用 ICF 转换的 PDD 与蒙特卡罗计算的 PDD 吻合良好。在不均匀介质中进行电离室剂量测量时,应严格考虑电离室扰动量校正和 SPR。在肺和骨材料的小射野剂量测量中,这一点更为重要。

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