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用于俄歇电子剂量测定和放射治疗的单色束表征

Monochromatic beam characterization for Auger electron dosimetry and radiotherapy.

作者信息

Dugas Joseph P, Oves Scott D, Sajo Erno, Matthews Kenneth L, Ham Kyungmin, Hogstrom Kenneth R

机构信息

Department of Physics and Astronomy, Louisiana State University, 202 Nicholson Hall, Baton Rouge, LA 70803, USA.

出版信息

Eur J Radiol. 2008 Dec;68(3 Suppl):S137-41. doi: 10.1016/j.ejrad.2008.04.050. Epub 2008 Jul 2.

Abstract

Dosimetry for Auger electron radiotherapy using monochromatic photon beams requires knowledge of beam characteristics. This study characterized a 35-keV photon beam generated at the LSU/CAMD synchrotron. Beam energy was measured by Compton spectroscopy and Si640c powder diffraction. Photon spatial distribution and virtual source position were measured using radiochromic film. Central-axis fluence was determined from Compton scattering measurements and application of the Klein-Nishina cross-section with percent polarization fit to results at 2-4 scattering angles. Broad-beam fluence was combined with MCNP5 Monte Carlo dose per fluence calculations to generate dose versus depth in a polymethylmethacrylate phantom, which was compared to ionization chamber and radiochromic film depth-dose measurements. For 22-41 keV beams, diffraction-based and Compton-based energy measurements agreed to within -0.1+/-0.3 and 0.6+/-0.3 keV, respectively, of monochromator calibrated energies. At 35 eV and 0.66 cm depth, dose uniformity over 80% of the 2.8 cm x 2.5 cm beam varied from 105 to 78% of the central-axis value horizontally and from 90 to 100% vertically. Narrow-beam divergence yielded vertical and horizontal virtual source-to-surface distances of 3.8+/-0.2 and 15.7+/-1.0m, respectively. Incident fluence rates for a 35-keV beam (100 mA ring current) ranged from 1.181+/-0.011 x 10(11) to 3.053+/-0.004 x 10(11)photons cm(-2)s(-1) with approximately 100% polarization in the horizontal plane. Ion chamber and film dose measurements underestimated MCNP5-based dose by an average of 6.4+/-0.8 and 9.1+/-0.8%, respectively, over measured depths. These practical beam characterization methods should allow subsequent Monte Carlo dose calculations needed for planning future radiotherapy studies. Although simulated and measured depth-dose curves agree well in shape, improvement in absolute dose is desirable.

摘要

使用单色光子束进行俄歇电子放射治疗的剂量测定需要了解束流特性。本研究对在路易斯安那州立大学/先进微结构材料中心(LSU/CAMD)同步加速器产生的35千电子伏特光子束进行了特性描述。束流能量通过康普顿光谱法和Si640c粉末衍射法进行测量。使用放射变色薄膜测量光子空间分布和虚拟源位置。中心轴注量由康普顿散射测量结果以及应用克莱因-仁科截面并对2至4个散射角的结果进行极化百分比拟合来确定。宽束注量与MCNP5蒙特卡罗每注量剂量计算结果相结合,以生成聚甲基丙烯酸甲酯体模中的剂量与深度关系,该结果与电离室和放射变色薄膜深度剂量测量结果进行了比较。对于22至41千电子伏特的束流,基于衍射和基于康普顿的能量测量结果分别与单色仪校准能量在-0.1±0.3千电子伏特和0.6±0.3千电子伏特范围内相符。在35电子伏特和0.66厘米深度处,在2.8厘米×2.5厘米束流的80%范围内,剂量均匀性在水平方向上为中心轴值的105%至78%,在垂直方向上为90%至100%。窄束发散导致垂直和水平方向上虚拟源到表面的距离分别为3.8±0.2米和15.7±1.0米。对于35千电子伏特的束流(环电流为100毫安),入射注量率范围为1.181±0.011×10¹¹至3.053±0.004×10¹¹光子·厘米⁻²·秒⁻¹,在水平平面内极化率约为100%。在测量深度范围内,电离室和薄膜剂量测量结果分别比基于MCNP5的剂量低估了6.4±0.8%和9.1±0.8%。这些实用的束流特性描述方法应能满足未来放射治疗研究规划所需的后续蒙特卡罗剂量计算。尽管模拟和测量的深度剂量曲线在形状上吻合良好,但绝对剂量仍有待改进。

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