Knesaurek K, Machac J
Division of Nuclear Medicine, Mount Sinai Medical Center, New York, New York, USA.
J Nucl Med. 1997 Dec;38(12):1992-8.
We developed and tested a new transformation cross-talk correction method for simultaneous dual-isotope SPECT imaging, which uses information from three energy windows in a simultaneous 18F/99mTc cardiac phantom study.
The method combines the previously reported "three-window" technique and transformation cross-talk correction methods. In the three-window technique, the images from the third energy "scatter" window are usually multiplied by a constant factor to obtain the estimates of the cross-talk. However, such an approach neglects differences in the spatial distribution between cross-talk photons in different energy windows. The transformation method is based on the assumption that the transformations, which convert the images from one energy window into the other energy windows, are known. These transformations were found by measuring the point-spread functions in different energy windows for both isotopes in water. The transformation method takes into account the different spatial distributions of the primary and scatter cross-talk photons in the different energy windows. Here, we are assuming that the imaging system and the image transformations between different energy windows are shift-invariant and linear. Thus, the new method is described by two convolution equations applied in frequency space. In addition to the cross-talk correction, the restoration filters were also applied to the resulting corrected images. The new method was performed on the simultaneous 18F/99mTc cardiac phantom study. Three separate studies were acquired in our phantom study: two single-isotope studies and one dual-isotope study. The single-isotope images were used as references. The contrast between the left ventricle cavity and the myocardium was used in transaxial slices as a parameter to evaluate results of the dual-isotope correction method with restoration.
The contrast improvement in the dual-isotope corrected images in both energy windows, i.e., the 99mTc primary window (140 keV) and the 18F primary window (511 keV), was significant. The corrected 511-keV, dual-isotope image had a contrast of 0.74 compared to 0.60, which was the value in the noncorrected dual-isotope image. The improvement of the contrast in the corrected, dual-isotope 511-keV image was exclusively a result of the restoration correction. The restoration-corrected, 511-keV, single-isotope 18F image had the same contrast (0.74). For the dual-isotope, 140-keV transaxial slice, first, the contrast improved from 0.78 to 0.85 after cross-talk correction, and, then, it finally reached 0.92 after additional restoration correction. The contrast in the 140-keV, single-isotope 99mTc image after restoration correction improved from 0.87 to 0.95.
The three-window transformation dual-isotope correction method with restoration significantly improves the contrast between the left ventricle cavity and the myocardium of the simultaneous 18F/99mTc SPECT imaging.
我们开发并测试了一种用于同时双同位素SPECT成像的新型变换串扰校正方法,该方法在同时进行的18F/99mTc心脏模型研究中使用了来自三个能量窗的信息。
该方法结合了先前报道的“三窗”技术和变换串扰校正方法。在三窗技术中,来自第三能量“散射”窗的图像通常乘以一个常数因子以获得串扰的估计值。然而,这种方法忽略了不同能量窗中串扰光子之间空间分布的差异。变换方法基于这样的假设,即已知将一个能量窗中的图像转换为其他能量窗中的图像的变换。通过测量水中两种同位素在不同能量窗中的点扩散函数来找到这些变换。变换方法考虑了不同能量窗中主串扰光子和散射串扰光子的不同空间分布。在此,我们假设成像系统以及不同能量窗之间的图像变换是平移不变且线性的。因此,新方法由在频率空间中应用的两个卷积方程描述。除了串扰校正之外,还对得到的校正图像应用了恢复滤波器。新方法应用于同时进行的18F/99mTc心脏模型研究。在我们的模型研究中进行了三项单独的研究:两项单同位素研究和一项双同位素研究。单同位素图像用作参考。在横断面切片中,左心室腔与心肌之间的对比度用作评估具有恢复功能的双同位素校正方法结果的参数。
在两个能量窗,即99mTc主窗(140 keV)和18F主窗(511 keV)中,双同位素校正图像的对比度均有显著提高。校正后的511 keV双同位素图像对比度为0.74,而未校正的双同位素图像对比度为0.60。校正后的双同位素511 keV图像对比度的提高完全是恢复校正的结果。恢复校正后的511 keV单同位素18F图像具有相同的对比度(0.74)。对于双同位素140 keV横断面切片,首先,串扰校正后对比度从0.78提高到0.85,然后,在额外的恢复校正后最终达到0.92。恢复校正后140 keV单同位素99mTc图像的对比度从0.87提高到0.95。
具有恢复功能的三窗变换双同位素校正方法显著提高了同时进行的18F/99mTc SPECT成像中左心室腔与心肌之间的对比度。