Cal-González J, Moore S C, Park M-A, Herraiz J L, Vaquero J J, Desco M, Udias J M
Grupo de Física Nuclear, Dpto. de Física Atómica, Molecular y Nuclear, Universidad Complutense de Madrid, CEI Moncloa, Spain.
Phys Med Biol. 2015 Sep 21;60(18):7127-49. doi: 10.1088/0031-9155/60/18/7127. Epub 2015 Sep 3.
In Positron Emission Tomography, there are several causes of quantitative inaccuracy, such as partial volume or spillover effects. The impact of these effects is greater when using radionuclides that have a large positron range, e.g. (68)Ga and (124)I, which have been increasingly used in the clinic. We have implemented and evaluated a local projection algorithm (LPA), originally evaluated for SPECT, to compensate for both partial-volume and spillover effects in PET. This method is based on the use of a high-resolution CT or MR image, co-registered with a PET image, which permits a high-resolution segmentation of a few tissues within a volume of interest (VOI) centered on a region within which tissue-activity values need to be estimated. The additional boundary information is used to obtain improved activity estimates for each tissue within the VOI, by solving a simple inversion problem. We implemented this algorithm for the preclinical Argus PET/CT scanner and assessed its performance using the radionuclides (18)F, (68)Ga and (124)I. We also evaluated and compared the results obtained when it was applied during the iterative reconstruction, as well as after the reconstruction as a postprocessing procedure. In addition, we studied how LPA can help to reduce the 'spillover contamination', which causes inaccurate quantification of lesions in the immediate neighborhood of large, 'hot' sources. Quantification was significantly improved by using LPA, which provided more accurate ratios of lesion-to-background activity concentration for hot and cold regions. For (18)F, the contrast was improved from 3.0 to 4.0 in hot lesions (when the true ratio was 4.0) and from 0.16 to 0.06 in cold lesions (true ratio = 0.0), when using the LPA postprocessing. Furthermore, activity values estimated within the VOI using LPA during reconstruction were slightly more accurate than those obtained by post-processing, while also visually improving the image contrast and uniformity within the VOI.
在正电子发射断层扫描(PET)中,存在多种导致定量不准确的原因,例如部分容积效应或溢出效应。当使用具有较大正电子射程的放射性核素时,这些效应的影响会更大,例如(68)Ga和(124)I,它们在临床上的使用越来越广泛。我们实施并评估了一种最初用于单光子发射计算机断层扫描(SPECT)的局部投影算法(LPA),以补偿PET中的部分容积效应和溢出效应。该方法基于使用与PET图像配准的高分辨率CT或MR图像,这允许对以需要估计组织活性值的区域为中心的感兴趣体积(VOI)内的几种组织进行高分辨率分割。通过解决一个简单的反演问题,利用额外的边界信息来获得VOI内每个组织的改进活性估计。我们在临床前的阿格斯PET/CT扫描仪上实现了该算法,并使用放射性核素(18)F、(68)Ga和(124)I评估了其性能。我们还评估并比较了在迭代重建期间应用该算法以及在重建后作为后处理程序时获得的结果。此外,我们研究了LPA如何有助于减少“溢出污染”,这种污染会导致对大的“热”源附近病变的定量不准确。使用LPA显著改善了定量,它为热区和冷区提供了更准确的病变与背景活性浓度比。对于(18)F,在使用LPA后处理时,热病变的对比度从3.0提高到4.0(真实比值为4.0),冷病变的对比度从0.16提高到0.06(真实比值 = 0.0)。此外,在重建期间使用LPA在VOI内估计的活性值比后处理获得的活性值略准确,同时在视觉上也改善了VOI内的图像对比度和均匀性。