Cherry S R, Meikle S R, Hoffman E J
Crump Institute, UCLA School of Medicine 90024-1721.
J Nucl Med. 1993 Apr;34(4):671-8.
Large sensitivity increases are realized in positron emission tomography when the interplane septa are removed and all lines of response acquired. Unfortunately, three-dimensional acquisition results in a large increase in scatter fraction which prevents accurate quantitation. By acquiring short two-dimensional scans prior to three-dimensional ones, scatter distributions can be estimated from differences between lines of response common to both datasets. This initial scatter distribution can be further modified to approximate scatter in the entire three-dimensional dataset. The method was validated with phantom measurements in which absolute activity concentrations were known in all compartments. Following scatter correction, a four-compartment phantom that was nonuniform in activity and density, both axially and transaxially, gave activity concentrations of 0.45 +/- 0.02, 0.31 +/- 0.02, 0.01 +/- 0.01 and 0.01 +/- 0.01 microCi/cc for compartments containing 0.43, 0.29, 0.0 (air) and 0.0 (water) microCi/cc, respectively. Thus, scatter distributions for complex sources can be estimated from image data without lengthy Monte-Carlo simulations. When activity distributions vary slowly with time, this method can be used to correct for scatter in three-dimensional patient studies.
当去除平面间隔板并获取所有响应线时,正电子发射断层扫描的灵敏度会大幅提高。不幸的是,三维采集会导致散射分数大幅增加,从而妨碍准确的定量分析。通过在三维扫描之前先进行短时间的二维扫描,可以根据两个数据集共有的响应线之间的差异来估计散射分布。这种初始散射分布可以进一步修正,以近似整个三维数据集的散射情况。该方法通过模型测量得到验证,其中所有隔室中的绝对活度浓度都是已知的。经过散射校正后,一个在轴向和横向活度及密度均不均匀的四隔室模型,对于分别含有0.43、0.29、0.0(空气)和0.0(水)微居里/立方厘米的隔室,其活度浓度分别为0.45±0.02、0.31±0.02、0.01±0.01和0.01±0.01微居里/立方厘米。因此,无需冗长的蒙特卡罗模拟,就可以从图像数据中估计复杂源的散射分布。当活度分布随时间缓慢变化时,该方法可用于校正三维患者研究中的散射。