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高能电子束在水中NACP - 02平行板电离室的扰动校正因子。

Perturbation correction factors for the NACP-02 plane-parallel ionization chamber in water in high-energy electron beams.

作者信息

Verhaegen F, Zakikhani R, Dusautoy A, Palmans H, Bostock G, Shipley D, Seuntjens J

机构信息

Medical Physics Department, McGill University, Montreal General Hospital, 1650 Cedar Avenue, Montreal, Québec H3G1A4, Canada.

出版信息

Phys Med Biol. 2006 Mar 7;51(5):1221-35. doi: 10.1088/0031-9155/51/5/012. Epub 2006 Feb 15.

Abstract

Recent dosimetry protocols for clinical high-energy electron beams recommend measurements of absorbed dose-to-water with a plane-parallel or cylindrical ionization chamber. For well-guarded plane-parallel ionization chambers, the ionization chamber perturbation factor in water, p(Q), has a recommended value of unity in all protocols. This assumption was investigated in detail in this study for one of the recommended ionization chambers in the protocols: the Scanditronix NACP-02 plane-parallel ionization chamber. Monte Carlo (MC) simulations of the NACP-02 ionization chamber with the EGSnrc code were validated against backscatter experiments. MC simulations were then used to calculate p(wall), p(cav) and p(Q) perturbation factors and water-to-air Spencer-Attix stopping powers in 4-19 MeV electron beams of a calibration laboratory (NPL), and in 6-22 MeV clinical electron beams from a Varian CL2300 accelerator. Differences between calculated and the currently recommended (Burns et al 1996 Med. Phys. 23 383-8) stopping powers, water-to-air, were found to be limited to 0.9% at depths between the reference depth z(ref) and the depth where the dose has decreased to 50% of the maximum dose, R50. p(wall) was found to exceed unity by 2.3% in the 4 MeV NPL calibration beam at z(ref). For higher energy electron beams p(wall) decreased to a value of about 1%. Combined with a p(cav) about 1% below unity for all energies at z(ref), this was found to cause p(Q) to exceed unity significantly for all energies. In clinical electron beams all three perturbation factors were found to increase with depth. Our findings indicate that the perturbation factors have to be taken into account in calibration procedures and for clinical depth dose measurements with the NACP-02 ionization chamber.

摘要

近期临床高能电子束剂量测定方案推荐使用平行板或圆柱形电离室测量水吸收剂量。对于防护良好的平行板电离室,在所有方案中,水中电离室扰动因子p(Q)的推荐值均为1。本研究针对方案中推荐的一种电离室——Scanditronix NACP - 02平行板电离室,详细研究了这一假设。利用EGSnrc代码对NACP - 02电离室进行蒙特卡罗(MC)模拟,并与反向散射实验进行了验证。然后,MC模拟用于计算校准实验室(NPL)4 - 19 MeV电子束以及Varian CL2300加速器6 - 22 MeV临床电子束中的p(wall)、p(cav)和p(Q)扰动因子以及水对空气的斯宾塞 - 阿蒂克斯阻止本领。计算得到的与当前推荐值(Burns等人,1996年,《医学物理》23卷,383 - 388页)的水对空气阻止本领之间的差异,发现在参考深度z(ref)与剂量降至最大剂量50%的深度R50之间的深度处,限制在0.9%以内。发现在z(ref)处,4 MeV NPL校准束中的p(wall)超过1达2.3%。对于更高能量的电子束,p(wall)降至约1%的值。结合在z(ref)处所有能量下约比1低1%的p(cav),发现这会导致所有能量下的p(Q)显著超过1。在临床电子束中,发现所有三个扰动因子均随深度增加。我们的研究结果表明,在校准程序以及使用NACP - 02电离室进行临床深度剂量测量时,必须考虑扰动因子。

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