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瓦里安、西门子、医科达和通用电气直线加速器的中子源强度测量

Neutron source strength measurements for Varian, Siemens, Elekta, and General Electric linear accelerators.

作者信息

Followill David S, Stovall Marilyn S, Kry Stephen F, Ibbott Geoffrey S

机构信息

Department of Radiation Physics, The University of Texas M. D. Anderson Cancer Center, 1515 Holcombe Boulevard, Houston, Texas 77030, USA.

出版信息

J Appl Clin Med Phys. 2003 Summer;4(3):189-94. doi: 10.1120/jacmp.v4i3.2514.

Abstract

The shielding calculations for high energy (>10 MV) linear accelerators must include the photoneutron production within the head of the accelerator. Procedures have been described to calculate the treatment room door shielding based on the neutron source strength (Q value) for a specific accelerator and energy combination. Unfortunately, there is currently little data in the literature stating the neutron source strengths for the most widely used linear accelerators. In this study, the neutron fluence for 36 linear accelerators, including models from Varian, Siemens, Elekta/Philips, and General Electric, was measured using gold-foil activation. Several of the models and energy combinations had multiple measurements. The neutron fluence measured in the patient plane was independent of the surface area of the room, suggesting that neutron fluence is more dependent on the direct neutron fluence from the head of the accelerator than from room scatter. Neutron source strength, Q, was determined from the measured neutron fluences. As expected, Q increased with increasing photon energy. The Q values ranged from 0.02 for a 10 MV beam to 1.44(x10(12)) neutrons per photon Gy for a 25 MV beam. The most comprehensive set of neutron source strength values, Q, for the current accelerators in clinical use are presented for use in calculating room shielding.

摘要

高能(>10 MV)直线加速器的屏蔽计算必须考虑加速器头部产生光中子的情况。已描述了根据特定加速器和能量组合的中子源强度(Q值)来计算治疗室门屏蔽的程序。遗憾的是,目前文献中几乎没有关于最常用直线加速器中子源强度的数据。在本研究中,使用金箔活化法测量了36台直线加速器的中子注量,这些加速器包括瓦里安、西门子、医科达/飞利浦和通用电气的型号。其中几种型号和能量组合进行了多次测量。在患者平面测量的中子注量与房间表面积无关,这表明中子注量更多地取决于加速器头部的直接中子注量,而非房间散射。根据测量的中子注量确定了中子源强度Q。正如预期的那样,Q随光子能量的增加而增加。Q值范围从10 MV束流的0.02到25 MV束流的每光子Gy 1.44×10¹²个中子。给出了目前临床使用的加速器最全面的中子源强度值Q集,用于计算房间屏蔽。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/587f/5724447/08184e907e33/ACM2-4-189-g001.jpg

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