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An investigation of gantry angle data accuracy for cine‐mode EPID images acquired during arc IMRT

机译:在电弧IMRT期间获取的电影模式EPID图像的龙门角度数据准确性的研究

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摘要

EPID images acquired in cine mode during arc therapy have inaccurate gantry angles recorded in their image headers. In this work, methods were developed to assess the accuracy of the gantry potentiometer for linear accelerators. As well, assessments of the accuracy of other, more accessible, sources of gantry angle information (i.e., treatment log files, analysis of EPID image headers) were investigated. The methods used in this study are generally applicable to any linear accelerator unit, and have been demonstrated here with Clinac/Trilogy systems. Gantry angle data were simultaneously acquired using three methods: i) a direct gantry potentiometer measurement, ii) an incremental rotary encoder, and iii) a custom‐made radiographic gantry‐angle phantom which produced unique wire intersections as a function of gantry angle. All methods were compared to gantry angle data from the EPID image header and the linac MLC DynaLog file. The encoder and gantry‐angle phantom were used to validate the accuracy of the linac's potentiometer. The EPID image header gantry angles and the DynaLog file gantry angles were compared to the potentiometer. The encoder and gantry‐angle phantom mean angle differences with the potentiometer were 0.13±0.14 and 0.10±0.30, respectively. The EPID image header angles analyzed in this study were within ±1 of the potentiometer angles only 35% of the time. In some cases, EPID image header gantry angles disagreed by as much as 3° with the potentiometer. A time delay in frame acquisition was determined using the continuous acquisition mode of the EPID. After correcting for this time delay, 75% of the header angles, on average, were within ±1 of the true gantry angle, compared to an average of only 35% without the correction. Applying a boxcar smoothing filter to the corrected gantry angles further improved the accuracy of the header‐derived gantry angles to within ±1 for almost all images (99.4%). An angle accuracy of 0.11±0.04 was determined using a point‐by‐point comparison of the gantry angle data in the MLC DynaLog file and the potentiometer data. These simple correction methods can be easily applied to individual treatment EPID images in order to more accurately define the gantry angle.PACS numbers: 87.53.Kn, 87.55.T‐, 87.56.bd, 87.59.‐e
机译:在弧光治疗期间以电影模式获取的EPID图像在其图像标题中记录了不正确的机架角度。在这项工作中,开发了评估直线加速器龙门电位器精度的方法。同样,还研究了其他更易于访问的龙门角度信息源(即治疗日志文件,EPID图像标题分析)的准确性评估。本研究中使用的方法通常适用于任何线性加速器单元,并且已在Clinac / Trilogy系统中进行了演示。使用三种方法同时获取龙门架角度数据:i)直接龙门架电位计测量; ii)增量式旋转编码器; iii)定制的射线照相龙门架角度体模,其产生的独特导线交叉点是龙门架角度的函数。将所有方法与来自EPID图像标题和直线加速器MLC DynaLog文件的龙门角度数据进行了比较。编码器和龙门架幻象用于验证直线加速器电位计的精度。将EPID图像标头龙门角度和DynaLog文件龙门角度与电位计进行了比较。编码器和机架角度幻像与电位计的平均角度差为 0.13 ± 0.14 0.10 ± 0.30 。本研究中分析的EPID图像标头角度在 <电位器角度的mo>± 1 仅为电位器角度的35%时间。在某些情况下,EPID图像标头龙门架角度与电位计相差3°之多。使用EPID的连续采集模式确定帧采集中的时间延迟。校正此时间延迟后,平均标题角的75%平均在 ± 1 真正的龙门角度,而未经校正的平均值仅为35%。将Boxcar平滑滤波器应用于校正后的龙门角度可进一步将标头衍生的龙门角度的精度提高到 ± 1 < / math>用于几乎所有图像(99.4%)。 0.11 < /mn>±0.04 是通过对MLC DynaLog文件中的龙门角度数据和电位计数据进行逐点比较确定的。这些简单的校正方法可以轻松地应用于各个处理的EPID图像,以更准确地定义龙门架角度.PACS编号:87.53.Kn,87.55.T-,87.56.bd,87.59.-e

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