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Characterization of a high-elbow, fluoroscopic electronic portal imaging device for portal dosimetry.

机译:用于门道剂量测定的高肘荧光透视电子门道成像设备的特性。

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摘要

The application of a newly developed fluoroscopic (CCD-camera based) electronic portal imaging device (EPID) in portal dosimetry is investigated. A description of the EPID response to dose is presented in terms of stability, linearity and optical cross-talk inside the mechanical structure. The EPID has a relatively large distance (41 cm on-axis) between the fluorescent screen and the mirror (high-elbow), which results in cross-talk with properties quite different from that of the low-elbow fluoroscopic EPIDs that have been studied in the literature. In contrast with low elbow systems, the maximum cross-talk is observed for points of the fluorescent screen that have the largest distance to the mirror, which is explained from the geometry of the system. An algorithm to convert the images of the EPID into portal dose images (PDIs) is presented. The correction applied for cross-talk is a position dependent additive operation on the EPID image pixel values, with a magnitude that depends on a calculated effective field width. Deconvolution with a point spread function, as applied for low-elbow systems, is not required. For a 25 MV beam, EPID PDIs and ionization chamber measurements in the EPID detector plane were obtained behind an anthropomorphic phantom and a homogeneous absorber for various field shapes. The difference in absolute dose between the EPID and ionization chamber measurements, averaged over the four test fields presented in this paper, was 0.1 +/- 0.5% (1 SD) over the entire irradiation field, with no deviation larger than 2%.
机译:研究了新开发的荧光镜(基于CCD相机)电子门成像设备(EPID)在门剂量中的应用。关于EPID对剂量的响应的描述是根据机械结构内部的稳定性,线性和光学串扰来进行的。 EPID在荧光屏和反射镜(高弯头)之间具有相对较大的距离(轴上为41 cm),这导致串扰的性质与已研究的低弯头荧光镜EPID完全不同在文学中。与低弯头系统相反,对于荧光镜的与反射镜具有最大距离的点,观察到最大的串扰,这可以从系统的几何形状中得到解释。提出了一种将EPID图像转换成门剂量图像(PDI)的算法。应用于串扰的校正是对EPID图像像素值的位置相关的加法运算,其大小取决于计算出的有效场宽。低弯头系统不需要使用带点扩展功能的反卷积。对于25 MV光束,在拟人体模和均质吸收体后面获得了针对各种场形的EPID PDI和EPID检测器平面中电离室的测量值。在本文介绍的四个测试场上,EPID和电离室测量值之间的绝对剂量差异在整个辐照场上平均为0.1 +/- 0.5%(1 SD),偏差不大于2%。

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