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正电子发射断层扫描/计算机断层扫描成像在放射治疗中的应用:一项用于设定生物靶区内部靶区体积的模体研究。

The use of positron emission tomography/computed tomography imaging in radiation therapy: a phantom study for setting internal target volume of biological target volume.

作者信息

Kawakami Wataru, Takemura Akihiro, Yokoyama Kunihiko, Nakajima Kenichi, Yokoyama Syoichi, Koshida Kichiro

机构信息

Department of Radiological Technology, Public Central Hospital of Matto Ishikawa, 3-8, Kuramitsu, Hakusan City, Ishikawa Pref, 924-8588, Japan.

Department of Quantum Medical Technology, Division of Health Sciences, Graduate School of Medical Science, Kanazawa University, Ishikawa, Japan.

出版信息

Radiat Oncol. 2015 Jan 8;10:1. doi: 10.1186/s13014-014-0315-2.

Abstract

BACKGROUND

Fluorodeoxyglucose ((18)F-FDG) positron emission tomography/computed tomography (PET/CT) is an important method for detecting tumours, planning radiotherapy treatment, and evaluating treatment responses. However, using the standardized uptake value (SUV) threshold with PET imaging may be suitable not to determine gross tumour volume but to determine biological target volume (BTV). The aim of this study was to extract internal target volume of BTV from PET images.

METHODS

Three spherical densities of (18)F-FDG were employed in a phantom with an air or water background with repetitive motion amplitudes of 0-30 mm. The PET data were reconstructed with attenuation correction (AC) based on CT images obtained by slow CT scanning (SCS) or helical CT scanning (HCS). The errors in measured SUVmax and volumes calculated using SUV threshold values based on SUVmax (THmax) in experiments performed with varying extents of respiratory motion and AC were analysed.

RESULTS

A partial volume effect (PVE) was not observed in spheres with diameters of ≥ 28 mm. When calculating SUVmax and THmax, using SCS for AC yielded smaller variance than using HCS (p<0.05). For spheres of 37- and 28-mm diameters in the phantom with either an air or water background, significant differences were observed when mean THmax of 30-, 20-, or 10-mm amplitude were compared with the stationary conditions (p<0.05). The average THmax values for 37-mm and 28-mm spheres with an air background were 0.362 and 0.352 in non-motion, respectively, and the mean THmax values for 37-mm and 28-mm spheres with a water background were 0.404 and 0.387 in non-motion and 0.244 and 0.263 in motion, respectively. When the phantom background was air, regardless of sphere concentration or size, THmax was dependent only on motion amplitude.

CONCLUSIONS

We found that there was no PVE for spheres with ≥ 28-mm diameters, and differences between SUVmax and THmax were reduced by using SCS for AC. In the head-and-neck and the abdomen, the standard values of THmax were 0.25 and 0.40 with and without respiratory movement, respectively. In the lungs, the value of THmax became the approximate expression depending on motion amplitude.

摘要

背景

氟脱氧葡萄糖((18)F-FDG)正电子发射断层扫描/计算机断层扫描(PET/CT)是检测肿瘤、规划放射治疗以及评估治疗反应的重要方法。然而,在PET成像中使用标准化摄取值(SUV)阈值可能并不适合确定大体肿瘤体积,而是适合确定生物靶区(BTV)。本研究的目的是从PET图像中提取BTV的内部靶区体积。

方法

在具有空气或水背景的体模中采用三种(18)F-FDG球形密度,重复运动幅度为0 - 30毫米。基于通过慢速CT扫描(SCS)或螺旋CT扫描(HCS)获得的CT图像,对PET数据进行衰减校正(AC)重建。分析了在不同程度的呼吸运动和AC条件下进行的实验中,测量的SUVmax误差以及使用基于SUVmax的SUV阈值(THmax)计算的体积误差。

结果

在直径≥28毫米的球体中未观察到部分容积效应(PVE)。在计算SUVmax和THmax时,使用SCS进行AC产生的方差比使用HCS小(p<0.05)。对于体模中直径为37毫米和28毫米的球体,在空气或水背景下,将3起毫米、20毫米或10毫米幅度的平均THmax与静止条件进行比较时,观察到显著差异(p<0.05)。空气背景下37毫米和28毫米球体在非运动状态下的平均THmax值分别为0.362和0.352,水背景下37毫米和28毫米球体在非运动状态下的平均THmax值分别为0.404和0.387,在运动状态下分别为0.244和0.263。当体模背景为空气时,无论球体浓度或大小如何,THmax仅取决于运动幅度。

结论

我们发现直径≥28毫米的球体不存在PVE,并且使用SCS进行AC可减少SUVmax和THmax之间的差异。在头颈部和腹部,有呼吸运动和无呼吸运动时THmax的标准值分别为0.25和0.40。在肺部,THmax的值根据运动幅度成为近似表达式。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f790/4299814/480b51298e34/13014_2014_315_Fig1_HTML.jpg

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