Øen Silje Kjærnes, Aasheim Lars Birger, Eikenes Live, Karlberg Anna Maria
Department of Circulation and Medical Imaging, Norwegian University of Science and Technology, Postbox 8905, N-7491, Trondheim, Norway.
Department of Radiology and Nuclear Medicine, St. Olavs University Hospital, Olav Kyrres gt 17, N-7006, Trondheim, Norway.
EJNMMI Phys. 2019 Aug 5;6(1):16. doi: 10.1186/s40658-019-0251-1.
The technology of modern positron emission tomography (PET) systems continuously improving, and with it the possibility to detect smaller lesions. Since first introduced in 2010, the number of hybrid PET/magnetic resonance imaging (MRI) systems worldwide is constantly increasing. It is therefore important to assess and compare the image quality, in terms of detectability, between the PET/MRI and the well-established PET/computed tomography (CT) systems. For this purpose, a PET image quality phantom (Esser) with hot spheres, ranging from 4 to 20 mm in diameter, was prepared with fluorodeoxyglucose and sphere-to-background activity concentrations of 8:1 and 4:1, to mimic clinical conditions. The phantom was scanned on a PET/MRI and a PET/CT system for both concentrations to obtain contrast recovery coefficients (CRCs) and contrast-to-noise ratios (CNRs), for a range of reconstruction settings. The detectability of the spheres was scored by three human observers for both systems and concentrations and all reconstructions. Furthermore, the impact of acquisition time on CNR and observer detectability was investigated.
Reconstructions applying point-spread-function modeling (and time-of-flight for the PET/CT) yielded the highest CRC and CNR in general, and PET/CT demonstrated slightly higher values than PET/MRI for most sphere sizes. CNR was dependent on reconstruction settings and was maximized for 2 iterations, a pixel size of less than 2 mm and a 4 mm Gaussian filter. Acquisition times of 97 s (PET/MRI) and 150 s (PET/CT) resulted in similar total net true counts. For these acquisition times, the smallest detected spheres by the human observers in the 8:1 activity concentration was the 6-mm sphere with PET/MRI (CNR = 5.6) and the 5-mm sphere with PET/CT (CNR = 5.5). With an acquisition time of 180 s, the 5-mm sphere was also detected with PET/MRI (CNR = 5.8). The 8-mm sphere was the smallest detected sphere in the 4:1 activity concentration for both systems.
In this experimental study, similar detectability was found for the PET/MRI and the PET/CT, although for an increased acquisition time for the PET/MRI.
现代正电子发射断层扫描(PET)系统技术不断进步,检测更小病变的可能性也随之提高。自2010年首次引入以来,全球范围内混合型PET/磁共振成像(MRI)系统的数量不断增加。因此,评估和比较PET/MRI与成熟的PET/计算机断层扫描(CT)系统在可检测性方面的图像质量非常重要。为此,制备了一个带有直径为4至20毫米热球的PET图像质量体模(埃塞尔体模),用氟脱氧葡萄糖填充,球与背景的活度浓度分别为8:1和4:1,以模拟临床情况。在PET/MRI和PET/CT系统上对该体模的两种浓度进行扫描,以获得一系列重建设置下的对比恢复系数(CRC)和对比噪声比(CNR)。由三位人类观察者对两种系统、两种浓度以及所有重建图像中球的可检测性进行评分。此外,还研究了采集时间对CNR和观察者可检测性的影响。
一般来说,应用点扩散函数建模(PET/CT还应用飞行时间技术)的重建方法能产生最高的CRC和CNR,对于大多数球尺寸,PET/CT显示的值略高于PET/MRI。CNR取决于重建设置,在2次迭代、像素尺寸小于2毫米和4毫米高斯滤波器的情况下达到最大值。97秒(PET/MRI)和150秒(PET/CT)的采集时间产生的总净真计数相似。对于这些采集时间,在8:1活度浓度下,人类观察者在PET/MRI中检测到的最小球为6毫米球(CNR = 5.6),在PET/CT中为5毫米球(CNR = 5.5)。采集时间为180秒时,PET/MRI也能检测到5毫米球(CNR = 5.8)。在4:1活度浓度下,两种系统中检测到的最小球均为8毫米球。
在本实验研究中,发现PET/MRI和PET/CT的可检测性相似,尽管PET/MRI的采集时间有所增加。