三维PET双能量窗散射校正性能的能量窗选择与参数实现比较

V. Sossi, J. S. Barney, T. Oakes, T. Ruth
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引用次数: 1

摘要

作者研究了双能量窗(DEW)散射校正方法中能量窗选择的相关性(Grootoenk et al., 1991)。该方法在很大程度上依赖于幻影研究中需要估计的两个参数之间的差异,低能窗(LEW)和高能窗(HEW)中真实事件之间的比率(R/sub unsc/),以及散射事件的等效比率(R/sub sc/)。无论能量窗选择如何,R/sub unsc/的跨轴分布都相对平坦。然而,能量窗的选择对R/sub sc/的跨轴分布有很大的影响。由于DEW散射校正方法没有使用卷积技术,因此参数的空间变化可能导致散射校正图像的不均匀性。研究了能量窗的选择和R/sub sc/的确定对DEW散射校正精度和均匀性的影响。基于稳定性考虑,选择了100-350-850 keV和250-380-850 keV两组能量窗进行研究。采用了三种方法来实现散射校正估计中的R/sub sc/值:包含R/sub sc/的跨轴分布的阵列;在直径20厘米的中心区域取R/sub sc/平均值,得到一个恒定值;和一个与中心R/sub sc/值相对应的常数值。常数R/sub sc/的使用将两组能量窗的图像均匀性从使用R/sub sc/阵列时获得的30%以内提高到15%左右。均匀性估计在直径20厘米的区域内。均匀幻斑和冷点研究确定的散射校正精度在所有病例中都具有可比性。两组能量窗获得的数据经本归一化算法归一化后,其跨轴和轴向图像均匀性无显著差异。同样,两种情况下获得的精度具有可比性,这表明R/sub sc/的实现方法比能量窗的选择对DEW散射校正方法的性能影响更大。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Comparison of energy window choice and parameter implementation in dual energy window scatter correction performance in 3D PET
The authors have investigated the relevance of the energy window choice in the dual energy window (DEW) scatter correction method (Grootoenk et al., 1991). This method depends strongly on the difference between 2 parameters that need to be estimated from phantom studies, the ratio (R/sub unsc/) between the true events in the low energy window (LEW) and high energy window (HEW), and the equivalent ratio for the scattered events (R/sub sc/). The transaxial distribution of the R/sub unsc/ is relatively flat regardless of the energy window selection. However, the energy window choice considerably influences the transaxial distribution of R/sub sc/. Since the DEW scatter correction method does not make use of convolution techniques, spatial variations of parameters are expected to lead to nonuniformities in scatter corrected images. The authors have investigated the DEW scatter correction accuracy and uniformity as a function of energy window choice and determination of R/sub sc/. Based on stability considerations 2 sets of energy windows have been selected for study, 100-350-850 keV and 250-380-850 keV. Three methods to implement the R/sub sc/ values in the scatter correction estimate have been used: an array containing the transaxial distribution of R/sub sc/; a constant value obtained by averaging R/sub sc/, over the central 20 cm diameter region; and a constant value corresponding to the central R/sub sc/ value. The use of constant values for R/sub sc/ improved image uniformity for both sets of energy windows from within 30% obtained when the array for R/sub sc/ was used, to about 15%. The uniformity was estimated over a 20 cm diameter region. Scatter correction accuracy as determined from uniform phantom and cold spot studies was comparable in all cases. No significant difference in transaxial or axial image uniformity was observed between data obtained with the 2 sets of energy windows and normalized with the present normalization algorithm. Likewise the accuracy obtained in both cases was comparable, indicating that the implementation method of the R/sub sc/ is a more important factor in the DEW scatter correction method performance than the selection of energy windows.
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