Deasy J O, Almond P R, McEllistrem M T
James Graham Brown Cancer Center, Department of Radiation Oncology, University of Louisville, Kentucky 40202, USA.
Med Phys. 1996 May;23(5):675-84. doi: 10.1118/1.597817.
Electron energy spectra and angular distributions, including angular spreads, were measured using magnetic spectrometer techniques, at isocenter, for two clinical linear accelerators: one scanning beam machine, which achieves field flatness by scanning a pencil beam over the desired field at the patient plane, and one scattering foil machine, which disperses the electrons through a graded-thickness scattering foil. All measurements were made at isocenter (in the patient plane), in air, 1 m from the nominal accelerator source. The energy measurements were confined to electrons traveling along the central axis; any widely scattered electrons were effectively neglected. The energy spectra of the scanning beam machine are all of nearly Gaussian shape and energy full-width-at-half-maximum intensity (FWHM) of about 5% of the peak mean energy (denoted (E0)). The energy spectra of the scattering foil machine have a variety of forms as a function of energy, including even spectra with double peaks, and spectra which changed with time. The FWHM values ranged from 9%-22% of (E0). The angular spread measurements, at isocenter, yielded sigma theta (x) x (E0)* approximately 295 mrad-MeV for the scanning beam machine, and 346 mrad-MeV for the scattering foil machine, where sigma theta x denotes the standard deviation of the plane-projected angular distribution. These angular spreads are 30%-40% smaller than angular spreads reported by others on a very similar machine using the penumbra method. Possible causes of this discrepancy are discussed.
使用磁谱仪技术在等中心对两台临床直线加速器的电子能谱和角分布(包括角展宽)进行了测量:一台是扫描束机器,它通过在患者平面上所需的射野上扫描笔形束来实现射野平坦度;另一台是散射箔机器,它通过渐变厚度的散射箔使电子散射。所有测量均在等中心(患者平面)、空气中、距标称加速器源1米处进行。能量测量仅限于沿中心轴传播的电子;任何广泛散射的电子都被有效忽略。扫描束机器的能谱几乎都是高斯形状,能量半高宽强度(FWHM)约为峰值平均能量(记为(E0)*)的5%。散射箔机器的能谱根据能量有多种形式,包括双峰的均匀能谱以及随时间变化的能谱。FWHM值范围为(E0)*的9% - 22%。在等中心的角展宽测量中,扫描束机器的σθx(E0)*约为295毫弧度 - 兆电子伏特,散射箔机器的为346毫弧度 - 兆电子伏特,其中σθx表示平面投影角分布的标准差。这些角展宽比其他人在使用半值层法的非常相似的机器上报告的角展宽小30% - 40%。讨论了这种差异的可能原因。